Waveguide device, and antenna device including the waveguide device

ABSTRACT

A waveguide device includes an electrical conductor including an electrically conductive surface, a waveguide extending alongside the electrically conductive surface, and an artificial magnetic conductor extending on both sides of the waveguide. The waveguide includes a first portion extending in one direction, and at least two branches extending from one end of the first portion, the at least two branches including a second portion and a third portion that extend in mutually different directions. A waveguide defined by the electrically conductive surface, the waveguide surface, and the artificial magnetic conductor includes an enlarged gap portion at which a gap between the electrically conductive surface and the waveguide surface is locally enlarged.

This is a continuation of PCT Application No. PCT/JP2018/017976, filed on May 9, 2018, and priority under 35 U.S.C. § 119(a) and 35 U.S.C. § 365(b) is claimed from Japanese Application No. 2017-094677, filed May 11, 2017, the entire contents of which are incorporated herein by reference.

1. FIELD OF THE INVENTION

The present disclosure relates to a waveguide device, and an antenna device including the waveguide device.

2. BACKGROUND

Examples of waveguiding structures including an artificial magnetic conductor are disclosed in the specification of U.S. Pat. No. 8,779,995, the specification of U.S. Pat. No. 8,803,638, the specification of European Patent and H. Kirino and K. Ogawa, “A 76 GHz Multi-Layered Phased Array Antenna using a Non-Metal Contact Metamaterial Waveguide”, IEEE Transaction on Antenna and Propagation, Vol. 60, No. 2, pp. 840-853, February, 2012, A. Uz. Zaman and P.-S. Kildal, “Ku Band Linear Slot-Array in Ridge Gapwaveguide Technology, EUCAP 2013, 7th European, A. Uz. Zaman and P.-S. Kildal, “Slot Antenna in Ridge Gap Waveguide Technology,” 6th European Conference on Antennas and Propagation, Prague, March, 2012. An artificial magnetic conductor is a structure which artificially realizes the properties of a perfect magnetic conductor (PMC), which does not exist in nature. One property of a perfect magnetic conductor is that “a magnetic field on its surface has zero tangential component”. This property is the opposite of the property of a perfect electric conductor (PEC), i.e., “an electric field on its surface has zero tangential component”. Although no perfect magnetic conductor exists in nature, it can be embodied by an artificial structure, e.g., an array of a plurality of electrically conductive rods. An artificial magnetic conductor functions as a perfect magnetic conductor in a specific frequency band which is defined by its structure. An artificial magnetic conductor restrains or prevents an electromagnetic wave of any frequency that is contained in the specific frequency band (propagation-restricted band) from propagating along the surface of the artificial magnetic conductor. For this reason, the surface of an artificial magnetic conductor may be referred to as a high impedance surface.

In the waveguide devices disclosed in the specification of U.S. Pat. No. 8,779,995, the specification of U.S. Pat. No. 8,803,638, the specification of European Patent and H. Kirino and K. Ogawa, “A 76 GHz Multi-Layered Phased Array Antenna using a Non-Metal Contact Metamaterial Wavegude”, IEEE Transaction on Antenna and Propagation, Vol. 60, No. 2, pp. 840-853, February, 2012, A. Uz. Zaman and P.-S. Kildal, “Ku Band Linear Slot-Array in Ridge Gapwaveguide Technology, EUCAP 2013, 7th European, A. Uz. Zaman and P.-S. Kildal, “Slot Antenna in Ridge Gap Waveguide Technology,” 6th European Conference on Antennas and Propagation, Prague, March, 2012, an artificial magnetic conductor is realized by a plurality of electrically conductive rods which are arrayed along row and column directions. Such rods are projections which may also be referred to as posts or pins. Each of these waveguide devices includes, as a whole, a pair of opposing electrically conductive plates. One conductive plate has a ridge protruding toward the other conductive plate, and stretches of an artificial magnetic conductor extending on both sides of the ridge. An upper face (i.e., its electrically conductive face) of the ridge opposes, via a gap, a conductive surface of the other conductive plate. An electromagnetic wave of a wavelength which is contained in the propagation-restricted band of the artificial magnetic conductor propagates along the ridge, in the space (gap) between this conductive surface and the upper face of the ridge.

SUMMARY

In a waveguide such as an antenna feeding network, branching portions may be provided on a waveguide. At a branching portion, the direction that the waveguide extends branches out into two or more. At such a branching portion, an impedance mismatch will occur unless some countermeasure is taken, thus resulting in unwanted reflection of an electromagnetic wave to propagate. Such reflection not only causes propagation losses of signals, but may also cause unwanted noises.

An example embodiment of the present disclosure provides a waveguide device in which a degree of impedance matching at any branching portion of a waveguide is enhanced.

A waveguide device according to one example embodiment of the present application includes an electrical conductor including an electrically conductive surface, a waveguide including an electrically-conductive waveguide surface opposed to the electrically conductive surface, and extending alongside the electrically conductive surface, and an artificial magnetic conductor extending on two sides of the waveguide. The waveguide includes a first portion extending in one direction, and at least two branches extending from one end of the first portion, the at least two branches including a second portion and a third portion that extend in mutually different directions. A waveguide which is defined by the electrically conductive surface, the waveguide surface, and the artificial magnetic conductor includes an enlarged gap portion at which a gap between the electrically conductive surface and the waveguide surface is locally enlarged. The size of the gap between the electrically conductive surface and the waveguide surface is greater at the enlarged gap portion than at any site on the waveguide that is adjacent to the enlarged gap portion, and is smaller than a distance between the electrically conductive surface and a root of the waveguide. At least a portion of a junction at which the first portion becomes jointed with the at least two branches of the waveguide overlaps the gap enlargement, as seen through in a direction perpendicular to the electrically conductive surface.

According to an example embodiment of the present disclosure, in at least a portion of a branching portion of a waveguide, a gap between a waveguide surface, and an electrically conductive surface is enlarged. As a result, the degree of impedance matching at the branching portion of the waveguide is enhanced.

The above and other elements, features, steps, characteristics and advantages of the present disclosure will become more apparent from the following detailed description of the example embodiments with reference to the attached drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a perspective view schematically showing a non-limiting example embodiment of a waveguide device according to the present disclosure.

FIG. 2A is a diagram schematically showing an example embodiment of the present disclosure for a waveguide device 100, in a cross section parallel to the XZ plane.

FIG. 2B is a diagram schematically showing another example embodiment of the present disclosure for the waveguide device 100 in FIG. 1, in a cross section parallel to the XZ plane.

FIG. 3 is another perspective view schematically showing the construction of an example embodiment of the present disclosure of the waveguide device 100, illustrated so that the spacing between a conductive member 110 and a conductive member 120 is exaggerated for ease of understanding.

FIG. 4 is a diagram showing an exemplary range of dimension of each member in the structure shown in FIG. 2A.

FIG. 5A is a diagram schematically showing an electromagnetic wave that propagates in a narrow space, i.e., a gap between a waveguide surface 122 a of a waveguide member 122 and a conductive surface 110 a of the conductive member 110 according to an example embodiment of the present disclosure.

FIG. 5B is a diagram schematically showing a cross section of a hollow waveguide 130 according to an example embodiment of the present disclosure.

FIG. 5C is a cross-sectional view showing an example embodiment of the present disclosure in which two waveguide members 122 are provided on the conductive member 120.

FIG. 5D is a diagram schematically showing a cross section of a waveguide device according to an example embodiment of the present disclosure in which two hollow waveguides 130 are placed side-by-side.

FIG. 6A is a diagram schematically showing an example embodiment of an impedance conversion structure (impedance transformer) which is used in a microstrip line.

FIG. 6B is a diagram schematically showing an example embodiment of a microstrip line construction in which a notch is provided for width adjustment at a branching portion.

FIG. 7 is a perspective views schematically showing a portion of the structure of a waveguide device according to a comparative example of the present disclosure.

FIG. 8A is a perspective views schematically showing part of the structure of a waveguide device according to a comparative example of the present disclosure.

FIG. 8B is a diagram showing enlarged the structure near a branching portion 136 in FIG. 8A.

FIG. 9A is a perspective view schematically showing part of the construction of a waveguide device according to an example embodiment structured so that the distance between the waveguide surface 122 a of the waveguide member 122 and the conductive surface 110 a of the conductive member 110 is decreased at impedance transformers.

FIG. 9B is a diagram showing enlarged the construction near a branching portion 136 in FIG. 9A.

FIG. 10 is a diagram schematically showing a cross-sectional structure of the waveguide device in FIG. 9A as taken along a plane which passes through the first portion 122A of the waveguide member 122 and is parallel to the YZ plane.

FIG. 11 is a diagram showing an equivalent circuit of the waveguide structure in FIG. 9A.

FIG. 12A is a perspective view schematically showing a portion of the structure of a waveguide device according to Example Embodiment 1 of the present disclosure.

FIG. 12B is an upper plan view showing the waveguide device of FIG. 12A as viewed from the +Z direction.

FIG. 12C is a diagram showing the waveguide device of FIG. 12A as viewed from the +Y direction.

FIG. 12D is a view exclusively showing the waveguide member 122, out of the waveguide device of FIG. 12B.

FIG. 12E is a diagram showing a variant of the waveguide device shown in FIG. 12D.

FIG. 13 is a diagram showing an equivalent circuit of the ridge waveguide according to Example Embodiment 1.

FIG. 14A is a diagram showing an example embodiment of a waveguide device having a staircase-shaped impedance matching structure, as in the comparative example shown in FIG. 9A.

FIG. 14B is a diagram showing an example embodiment of a waveguide device having an impedance matching structure such that the width of the waveguide surface 122 a increases toward the branching portion 136, as in the comparative example shown in FIG. 8A.

FIG. 15A is a diagram showing still another variant of Example Embodiment 1.

FIG. 15B is a diagram showing still another variant of Example Embodiment 1.

FIG. 16A is a diagram showing still another variant of Example Embodiment 1.

FIG. 16B is a diagram showing still another variant of Example Embodiment 1.

FIG. 17A shows frequency dependence of the input reflection coefficient in the construction of the comparative example shown in FIG. 9A.

FIG. 17B shows frequency dependence of the input reflection coefficient in the example embodiment illustrated in FIG. 14A.

FIG. 18A is a perspective view schematically showing part of the structure of a waveguide device according to Example Embodiment 2 of the present disclosure.

FIG. 18B is an upper plan view showing the waveguide device of FIG. 18A as viewed along the Z direction.

FIG. 19 is a perspective view schematically showing part of the structure of a waveguide device according to Example Embodiment 3 of the present disclosure.

FIG. 20A is a perspective view schematically showing a portion of the structure of a waveguide device according to a variant of Example Embodiment 1.

FIG. 20B is an upper plan view showing the waveguide device of FIG. 20A as viewed from the +Z direction.

FIG. 21A is a perspective view schematically showing a portion of the structure of a waveguide device according to another variant of Example Embodiment 1.

FIG. 21B is an upper plan view showing the waveguide device of FIG. 21A as viewed from the +Z direction

FIG. 22A is a perspective view schematically showing part of the structure of a waveguide device according to Example Embodiment 4 of the present disclosure.

FIG. 22B is an upper plan view showing the waveguide device of FIG. 22A as viewed from the +Z direction.

FIG. 23A is an upper plan view showing enlarged only the waveguide member 122 in the structure shown in FIG. 22A.

FIG. 23B is an upper plan view showing a variant of Example Embodiment 4.

FIG. 24 is an upper plan view showing a waveguide device which includes a waveguide member 122 having three branches as viewed from the +Z direction, as another variant of Example Embodiment 4.

FIG. 25A is a perspective view showing part of the structure of a waveguide device according to still another variant of Example Embodiment 4.

FIG. 25B is an upper plan view showing the structure of FIG. 25A as viewed from the +Z direction.

FIG. 26A is a perspective view showing a portion of the structure of a waveguide device according to Example Embodiment 5 of the present disclosure.

FIG. 26B is an upper plan view showing the structure of FIG. 26A as viewed from the +Z direction.

FIG. 27 is a perspective view showing enlarged only a portion of the waveguide member 122 for ease of understanding

FIG. 28 is a diagram showing an equivalent circuit of a ridge waveguide according to Example Embodiment 5.

FIG. 29A is a cross-sectional view schematically showing another example embodiment of the impedance transformer.

FIG. 29B is a cross-sectional view schematically showing still another example embodiment of the impedance transformer.

FIG. 30A is a diagram showing an example embodiment where, as viewed in a direction perpendicular to the conductive surface 110 a, the dimension of a gap enlargement 141 along the width direction of the first portion 122A of the waveguide member decreases toward the first portion 122A.

FIG. 30B is a diagram showing an example embodiment where, as viewed in a direction perpendicular to the conductive surface 110 a, the dimension of a gap enlargement 141 along the width direction of the first portion 122A of the waveguide member increases toward the first portion 122A.

FIG. 30C is a diagram showing an example embodiment where a gap enlargement 141 of an elliptic shape is provided in a central portion of a branching portion of the waveguide member, without reaching the edge of any of the first portion 122A, the second portion 122B, or the third portion 122C.

FIG. 30D is a diagram showing an example embodiment where a gap enlargement 141 of a semicircular shape is located adjacent to an end of the first portion 122A of the waveguide member

FIG. 31A is a diagram showing still another variant of a waveguide device according to an example embodiment of the present disclosure.

FIG. 31B is a diagram showing still another variant of a waveguide device according to an example embodiment of the present disclosure.

FIG. 32A is an upper plan view of an array antenna according to an example embodiment of the present disclosure as viewed from the +Z direction.

FIG. 32B is a cross-sectional view taken along line B-B in FIG. 32A.

FIG. 33A is a diagram showing a planar layout of a waveguide member 122U of a first waveguide device 100 a according to an example embodiment of the present disclosure.

FIG. 33B is a diagram showing a planar layout of a waveguide member 122L of a second waveguide device 100 b according to an example embodiment of the present disclosure.

FIG. 34A is a cross-sectional view showing an example embodiment of the present disclosure where only a waveguide surface 122 a, defining an upper surface of the waveguide member 122, is electrically conductive, while any portion of the waveguide member 122 other than the waveguide surface 122 a is not electrically conductive.

FIG. 34B is a diagram showing an example embodiment of the present disclosure in which the waveguide member 122 is not on the conductive member 120.

FIG. 34C is a diagram showing an example embodiment where the conductive member 120, the waveguide member 122, and each of the plurality of conductive rods 124 are composed of a dielectric surface that is coated with an electrically conductive material such as a metal.

FIG. 34D is a diagram showing an example embodiment of the present disclosure in which dielectric layers 110 c and 120 c are respectively provided on the outermost surfaces of conductive members 110 and 120, a waveguide member 122, and conductive rods 124.

FIG. 34E is a diagram showing another example embodiment of the present disclosure in which dielectric layers 110 c and 120 c are respectively provided on the outermost surfaces of conductive members 110 and 120, a waveguide member 122, and conductive rods 124.

FIG. 34F is a diagram showing an example embodiment of the present disclosure where the height of the waveguide member 122 is lower than the height of the conductive rods 124 and a portion of a conductive surface 110 a of the conductive member 110 that opposes the waveguide surface 122 a protrudes toward the waveguide member 122.

FIG. 34G is a diagram showing an example embodiment of the present disclosure where, further in the structure of FIG. 34F, portions of the conductive surface 110 a that oppose the conductive rods 124 protrude toward the conductive rods 124.

FIG. 35A is a diagram showing an example embodiment of the present disclosure where a conductive surface 110 a of the conductive member 110 is shaped as a curved surface.

FIG. 35B is a diagram showing an example embodiment of the present disclosure where a conductive surface 120 a of the conductive member 120 is also shaped as a curved surface.

FIG. 36 is a diagram showing a driver's vehicle 500, and a preceding vehicle 502 that is traveling in the same lane as the driver's vehicle 500 according to an example embodiment of the present disclosure.

FIG. 37 is a diagram showing an onboard radar system 510 of the driver's vehicle 500.

FIG. 38A is a diagram showing a relationship between an array antenna AA of the onboard radar system 510 and plural arriving waves k according to an example embodiment of the present disclosure.

FIG. 38B is a diagram showing the array antenna AA receiving the k^(th) arriving wave.

FIG. 39 is a block diagram showing an example embodiment of a vehicle travel controlling apparatus 600 according to the present disclosure.

FIG. 40 is a block diagram showing another example embodiment of the present disclosure for the vehicle travel controlling apparatus 600.

FIG. 41 is a block diagram showing an example embodiment of the present disclosure of a more specific construction of the vehicle travel controlling apparatus 600.

FIG. 42 is a block diagram showing a more detailed example embodiment of the present disclosure of the radar system 510 according to this Application Example.

FIG. 43 is a diagram showing change in frequency of a transmission signal which is modulated based on the signal that is generated by a triangular wave generation circuit 581 according to an example embodiment of the present disclosure.

FIG. 44 is a diagram showing a beat frequency fu in an “ascent” period and a beat frequency fd in a “descent” period according to an example embodiment of the present disclosure.

FIG. 45 is a diagram showing an example embodiment of the present disclosure in which a signal processing circuit 560 is implemented in hardware including a processor PR and a memory device MD.

FIG. 46 is a diagram showing a relationship between three frequencies f1, f2 and f3 according to an example embodiment of the present disclosure.

FIG. 47 is a diagram showing a relationship between synthetic spectra F1 to F3 on a complex plane according to an example embodiment of the present disclosure.

FIG. 48 is a flowchart showing the procedure of a process of determining relative velocity and distance according to an example embodiment of the present disclosure.

FIG. 49 is a diagram concerning a fusion apparatus in which a radar system 510 having a slot array antenna and an onboard camera system 700 are included according to an example embodiment of the present disclosure.

FIG. 50 is a diagram illustrating how placing a millimeter wave radar 510 and a camera at substantially the same position within the vehicle room may allow them to acquire an identical field of view and line of sight, thus facilitating a matching process according to an example embodiment of the present disclosure.

FIG. 51 is a diagram showing an example embodiment of the present disclosure for a monitoring system 1500 based on millimeter wave radar.

FIG. 52 is a block diagram showing an example embodiment of the present disclosure for a digital communication system 800A.

FIG. 53 is a block diagram showing an example embodiment of the present disclosure of a communication system 800B including a transmitter 810B which is capable of changing its radio wave radiation pattern.

FIG. 54 is a block diagram showing an example embodiment of the present disclosure of a communication system 800C implementing a MIMO function.

DETAILED DESCRIPTION

Prior to describing example embodiments of the present disclosure, findings that form the basis of the present disclosure will be described.

A ridge waveguide which is disclosed in the aforementioned specification of U.S. Pat. No. 8,779,995, the specification of U.S. Pat. No. 8,803,638, the specification of European Patent Application Publication No. 1331688 and H. Kirino and K. Ogawa, “A 76 GHz Multi-Layered Phased Array Antenna using a Non-Metal Contact Metamaterial Wavegude”, IEEE Transaction on Antenna and Propagation, Vol. 60, No. 2, pp. 840-853, February, 2012 and A. Uz. Zaman and P.-S. Kildal, “Ku Band Linear Slot-Array in Ridge Gapwaveguide Technology, EUCAP 2013, 7th European Conference on Antenna and Propagation is provided in a waffle iron structure which is capable of functioning as an artificial magnetic conductor. A ridge waveguide in which such an artificial magnetic conductor is utilized based on the present disclosure (which hereinafter may be referred to as a WRG: Waffle-iron Ridge waveguide) is able to realize an antenna feeding network with low losses in the microwave or the millimeter wave band. Moreover, use of such a ridge waveguide allows antenna elements to be disposed with a high density. Hereinafter, an exemplary fundamental construction and operation of such a waveguide structure will be described.

An artificial magnetic conductor is a structure which artificially realizes the properties of a perfect magnetic conductor (PMC), which does not exist in nature. One property of a perfect magnetic conductor is that “a magnetic field on its surface has zero tangential component”. This property is the opposite of the property of a perfect electric conductor (PEC), i.e., “an electric field on its surface has zero tangential component”. Although no perfect magnetic conductor exists in nature, it can be embodied by an artificial structure, e.g., an array of a plurality of electrically conductive rods. An artificial magnetic conductor functions as a perfect magnetic conductor in a specific frequency band which is defined by its structure. An artificial magnetic conductor restrains or prevents an electromagnetic wave of any frequency that is contained in the specific frequency band (propagation-restricted band) from propagating along the surface of the artificial magnetic conductor. For this reason, the surface of an artificial magnetic conductor may be referred to as a high impedance surface.

In the waveguide devices disclosed in the specification of U.S. Pat. No. 8,779,995, the specification of U.S. Pat. No. 8,803,638, the specification of European Patent and H. Kirino and K. Ogawa, “A 76 GHz Multi-Layered Phased Array Antenna using a Non-Metal Contact Metamaterial Wavegude”, IEEE Transaction on Antenna and Propagation, Vol. 60, No. 2, pp. 840-853, February, 2012 and A. Uz. Zaman and P.-S. Kildal, “Ku Band Linear Slot-Array in Ridge Gapwaveguide Technology, EUCAP 2013, 7th European Conference on Antenna and Propagation, an artificial magnetic conductor is realized by a plurality of electrically conductive rods which are arrayed along row and column directions. Such rods are projections which may also be referred to as posts or pins. Each of these waveguide devices includes, as a whole, a pair of opposing electrically conductive plates. One conductive plate has a ridge protruding toward the other conductive plate, and stretches of an artificial magnetic conductor extending on both sides of the ridge. An upper face (i.e., its electrically conductive face) of the ridge opposes, via a gap, an electrically conductive surface of the other conductive plate. An electromagnetic wave (signal wave) of a wavelength which is contained in the propagation-restricted band of the artificial magnetic conductor propagates along the ridge, in the space (gap) between this conductive surface and the upper face of the ridge.

FIG. 1 is a perspective view schematically showing a non-limiting example of a fundamental construction of such a waveguide device. FIG. 1 shows XYZ coordinates along X, Y and Z directions which are orthogonal to one another. The waveguide device 100 shown in the figure includes a plate-like electrically conductive member 110 and a plate shape (plate-like) electrically conductive member 120, which are in opposing and parallel positions to each other. A plurality of electrically conductive rods 124 are arrayed on the second conductive member 120.

Note that any structure appearing in a figure of the present application is shown in an orientation that is selected for ease of explanation, which in no way should limit its orientation when an example embodiment of the present disclosure is actually practiced. Moreover, the shape and size of a whole or a part of any structure that is shown in a figure should not limit its actual shape and size.

FIG. 2A is a diagram schematically showing the construction of a cross section of the waveguide device 100 in FIG. 1, taken parallel to the XZ plane. As shown in FIG. 2A, the conductive member 110 has an electrically conductive surface 110 a on the side facing the conductive member 120. The conductive surface 110 a has a two-dimensional expanse along a plane which is orthogonal to the axial direction (i.e., the Z direction) of the conductive rods 124 (i.e., a plane which is parallel to the XY plane). Although the conductive surface 110 a is shown to be a smooth plane in this example, the conductive surface 110 a does not need to be a plane, as will be described later.

FIG. 3 is a perspective view schematically showing the waveguide device 100, illustrated so that the spacing between the conductive member 110 and the conductive member 120 is exaggerated for ease of understanding. In an actual waveguide device 100, as shown in FIG. 1 and FIG. 2A, the spacing between the conductive member 110 and the conductive member 120 is narrow, with the conductive member 110 covering over all of the conductive rods 124 on the conductive member 120.

FIG. 1 to FIG. 3 only show portions of the waveguide device 100. The conductive members 110 and 120, the waveguide member 122, and the plurality of conductive rods 124 actually extend to outside of the portions illustrated in the figures. At an end of the waveguide member 122, as will be described later, a choke structure for preventing electromagnetic waves from leaking into the external space is provided. The choke structure may include a row of conductive rods that are adjacent to the end of the waveguide member 122, for example.

See FIG. 2A again. The plurality of conductive rods 124 arrayed on the conductive member 120 each have a leading end 124 a opposing the conductive surface 110 a. In the example shown in the figure, the leading ends 124 a of the plurality of conductive rods 124 are on the same plane. This plane defines the surface 125 of an artificial magnetic conductor. Each conductive rod 124 does not need to be entirely electrically conductive, so long as it at least includes an electrically conductive layer that extends along the upper face and the side surface of the rod-like structure. Although this electrically conductive layer may be located at the surface layer of the rod-like structure, the surface layer may be composed of an insulation coating or a resin layer with no electrically conductive layer existing on the surface of the rod-like structure. Moreover, each conductive member 120 does not need to be entirely electrically conductive, so long as it can support the plurality of conductive rods 124 to constitute an artificial magnetic conductor. Of the surfaces of the conductive member 120, a face carrying the plurality of conductive rods 124 may be electrically conductive, such that the electrical conductor electrically interconnects the surfaces of adjacent ones of the plurality of conductive rods 124. Moreover, the electrically conductive layer of the conductive member 120 may be covered with an insulation coating or a resin layer. In other words, the entire combination of the conductive member 120 and the plurality of conductive rods 124 may at least include an electrically conductive layer with rises and falls opposing the conductive surface 110 a of the conductive member 110.

On the conductive member 120, a ridge-like waveguide member 122 is provided among the plurality of conductive rods 124. More specifically, stretches of an artificial magnetic conductor are present on both sides of the waveguide member 122, such that the waveguide member 122 is sandwiched between the stretches of artificial magnetic conductor on both sides. As can be seen from FIG. 3, the waveguide member 122 in this example is supported on the conductive member 120, and extends linearly along the Y direction. In the example shown in the figure, the waveguide member 122 has the same height and width as those of the conductive rods 124. As will be described later, however, the height and width of the waveguide member 122 may have respectively different values from those of the conductive rod 124. Unlike the conductive rods 124, the waveguide member 122 extends along a direction (which in this example is the Y direction) in which to guide electromagnetic waves along the conductive surface 110 a. Similarly, the waveguide member 122 does not need to be entirely electrically conductive, but may at least include an electrically conductive waveguide surface 122 a opposing the conductive surface 110 a of the conductive member 110. The conductive member 120, the plurality of conductive rods 124, and the waveguide member 122 may be portions of a continuous single-piece body. Furthermore, the conductive member 110 may also be a portion of such a single-piece body.

On both sides of the waveguide member 122, the space between the surface 125 of each stretch of artificial magnetic conductor and the conductive surface 110 a of the conductive member 110 does not allow an electromagnetic wave of any frequency that is within a specific frequency band to propagate. This frequency band is called a “prohibited band”. The artificial magnetic conductor is designed so that the frequency of an electromagnetic wave (signal wave) to propagate in the waveguide device 100 (which may hereinafter be referred to as the “operating frequency”) is contained in the prohibited band. The prohibited band may be adjusted based on the following: the height of the conductive rods 124, i.e., the depth of each groove formed between adjacent conductive rods 124; the width of each conductive rod 124; the interval between conductive rods 124; and the size of the gap between the leading end 124 a and the conductive surface 110 a of each conductive rod 124.

Next, with reference to FIG. 4, the dimensions, shape, positioning, and the like of each member will be described.

FIG. 4 is a diagram showing an exemplary range of dimension of each member in the structure shown in FIG. 2A. The waveguide device is used for at least one of transmission and reception of electromagnetic waves of a predetermined band (referred to as the “operating frequency band”). In the present specification, λo denotes a representative value of wavelengths in free space (e.g., a central wavelength corresponding to a center frequency in the operating frequency band) of an electromagnetic wave (signal wave) propagating in a waveguide extending between the conductive surface 110 a of the conductive member 110 and the waveguide surface 122 a of the waveguide member 122. Moreover, λm denotes a wavelength, in free space, of an electromagnetic wave of the highest frequency in the operating frequency band. The end of each conductive rod 124 that is in contact with the conductive member 120 is referred to as the “root”. As shown in FIG. 4, each conductive rod 124 has the leading end 124 a and the root 124 b. Examples of dimensions, shapes, positioning, and the like of the respective members are as follows.

(1) Width of the Conductive Rod

The width (i.e., the size along the X direction and the Y direction) of the conductive rod 124 may be set to less than λm/2. Within this range, resonance of the lowest order can be prevented from occurring along the X direction and the Y direction. Since resonance may possibly occur not only in the X and Y directions but also in any diagonal direction in an X-Y cross section, the diagonal length of an X-Y cross section of the conductive rod 124 is also preferably less than λm/2. The lower limit values for the rod width and diagonal length will conform to the minimum lengths that are producible under the given manufacturing method, but is not particularly limited.

(2) Distance from the Root of the Conductive Rod to the Conductive Surface of the Conductive Member 110

The distance from the root 124 b of each conductive rod 124 to the conductive surface 110 a of the conductive member 110 may be longer than the height of the conductive rods 124, while also being less than λm/2. When the distance is λm/2 or more, resonance may occur between the root 124 b of each conductive rod 124 and the conductive surface 110 a, thus reducing the effect of signal wave containment.

The distance from the root 124 b of each conductive rod 124 to the conductive surface 110 a of the conductive member 110 corresponds to the spacing between the conductive member 110 and the conductive member 120. For example, when a signal wave of 76.5±0.5 GHz (which belongs to the millimeter band or the extremely high frequency band) propagates in the waveguide, the wavelength of the signal wave is in the range from 3.8934 mm to 3.9446 mm. Therefore, λm equals 3.8934 mm in this case, so that the spacing between the conductive member 110 and the conductive member 120 may be set to less than a half of 3.8934 mm. So long as the conductive member 110 and the conductive member 120 realize such a narrow spacing while being disposed opposite from each other, the conductive member 110 and the conductive member 120 do not need to be strictly parallel. Moreover, when the spacing between the conductive member 110 and the conductive member 120 is less than λm/2, a whole or a part of the conductive member 110 and/or the conductive member 120 may be shaped as a curved surface. On the other hand, the conductive members 110 and 120 each have a planar shape (i.e., the shape of their region as perpendicularly projected onto the XY plane) and a planar size (i.e., the size of their region as perpendicularly projected onto the XY plane) which may be arbitrarily designed depending on the purpose.

Although the conductive surface 120 a is illustrated as a plane in the example shown in FIG. 2A, example embodiments of the present disclosure are not limited thereto. For example, as shown in FIG. 2B, the conductive surface 120 a may be the bottom parts of faces each of which has a cross section similar to a U-shape or a V-shape. The conductive surface 120 a will have such a structure when each conductive rod 124 or the waveguide member 122 is shaped with a width which increases toward the root. Even with such a structure, the device shown in FIG. 2B can function as the waveguide device according to an example embodiment of the present disclosure so long as the distance between the conductive surface 110 a and the conductive surface 120 a is less than a half of the wavelength λm.

(3) Distance L2 from the Leading End of the Conductive Rod to the Conductive Surface

The distance L2 from the leading end 124 a of each conductive rod 124 to the conductive surface 110 a is set to less than λm/2. When the distance is λm/2 or more, a propagation mode where electromagnetic waves reciprocate between the leading end 124 a of each conductive rod 124 and the conductive surface 110 a may occur, thus no longer being able to contain an electromagnetic wave. Note that, among the plurality of conductive rods 124, at least those which are adjacent to the waveguide member 122 do not have their leading ends in electrical contact with the conductive surface 110 a. As used herein, the leading end of a conductive rod not being in electrical contact with the conductive surface means either of the following states: there being an air gap between the leading end and the conductive surface; or the leading end of the conductive rod and the conductive surface adjoining each other via an insulating layer which may exist in the leading end of the conductive rod or in the conductive surface.

(4) Arrangement and Shape of Conductive Rods

The interspace between two adjacent conductive rods 124 among the plurality of conductive rods 124 has a width of less than λm/2, for example. The width of the interspace between any two adjacent conductive rods 124 is defined by the shortest distance from the surface (side surface) of one of the two conductive rods 124 to the surface (side surface) of the other. This width of the interspace between rods is to be determined so that resonance of the lowest order will not occur in the regions between rods. The conditions under which resonance will occur are determined based by a combination of: the height of the conductive rods 124; the distance between any two adjacent conductive rods; and the capacitance of the air gap between the leading end 124 a of each conductive rod 124 and the conductive surface 110 a. Therefore, the width of the interspace between rods may be appropriately determined depending on other design parameters. Although there is no clear lower limit to the width of the interspace between rods, for manufacturing ease, it may be e.g. λm/16 or more when an electromagnetic wave in the extremely high frequency range is to be propagated. Note that the interspace does not need to have a constant width. So long as it remains less than λm/2, the interspace between conductive rods 124 may vary.

The arrangement of the plurality of conductive rods 124 is not limited to the illustrated example, so long as it exhibits a function of an artificial magnetic conductor. The plurality of conductive rods 124 do not need to be arranged in orthogonal rows and columns; the rows and columns may be intersecting at angles other than 90 degrees. The plurality of conductive rods 124 do not need to form a linear array along rows or columns, but may be in a dispersed arrangement which does not present any straightforward regularity. The conductive rods 124 may also vary in shape and size depending on the position on the conductive member 120.

The surface 125 of the artificial magnetic conductor that are constituted by the leading ends 124 a of the plurality of conductive rods 124 does not need to be a strict plane, but may be a plane with minute rises and falls, or even a curved surface. In other words, the conductive rods 124 do not need to be of uniform height, but rather the conductive rods 124 may be diverse so long as the array of conductive rods 124 is able to function as an artificial magnetic conductor.

Each conductive rod 124 does not need to have a prismatic shape as shown in the figure, but may have a cylindrical shape, for example. Furthermore, each conductive rod 124 does not need to have a simple columnar shape. The artificial magnetic conductor may also be realized by any structure other than an array of conductive rods 124, and various artificial magnetic conductors are applicable to the waveguide device of the present disclosure. Note that, when the leading end 124 a of each conductive rod 124 has a prismatic shape, its diagonal length is preferably less than λm/2. When the leading end 124 a of each conductive rod 124 is shaped as an ellipse, the length of its major axis is preferably less than λm/2. Even when the leading end 124 a has any other shape, the dimension across it is preferably less than λm/2 even at the longest position.

The height of each conductive rod 124 (in particular, those conductive rods 124 which are adjacent to the waveguide member 122), i.e., the length from the root 124 b to the leading end 124 a, may be set to a value which is shorter than the distance (i.e., less than λm/2) between the conductive surface 110 a and the conductive surface 120 a, e.g., λo/4.

(5) Width of the Waveguide Surface

The width of the waveguide surface 122 a of the waveguide member 122, i.e., the size of the waveguide surface 122 a along a direction which is orthogonal to the direction that the waveguide member 122 extends, may be set to less than λm/2 (e.g. λo/8). If the width of the waveguide surface 122 a is λm/2 or more, resonance will occur along the width direction, which will prevent any WRG from operating as a simple transmission line.

(6) Height of the Waveguide Member

The height (i.e., the size along the Z direction in the example shown in the figure) of the waveguide member 122 is set to less than λm/2. The reason is that, if the distance is λm/2 or more, the distance between the root 124 b of each conductive rod 124 and the conductive surface 110 a will be λm/2 or more. Similarly, the height of each conductive rod 124 (in particular, any conductive rod 124 that is adjacent to the waveguide member 122) is also set to less than λm/2.

(7) Distance L1 Between the Waveguide Surface and the Conductive Surface

The distance L1 between the waveguide surface 122 a of the waveguide member 122 and the conductive surface 110 a is set to less than λm/2. If the distance is λm/2 or more, resonance will occur between the waveguide surface 122 a and the conductive surface 110 a, which will prevent functionality as a waveguide. In one example, the distance L1 is λm/4 or less. In order to ensure manufacturing ease, when an electromagnetic wave in the extremely high frequency range is to propagate, the distance L1 is preferably λm/16 or more, for example.

The lower limit of the distance L1 between the conductive surface 110 a and the waveguide surface 122 a and the lower limit of the distance L2 between the conductive surface 110 a and the leading end 124 a of each conductive rod 124 depends on the machining precision, and also on the precision when assembling the two upper/lower conductive members 110 and 120 so as to be apart by a constant distance. When a pressing technique or an injection technique is used, the practical lower limit of the aforementioned distance is about 50 micrometers (μm). In the case of using an MEMS (Micro-Electro-Mechanical System) technique to make a product in e.g. the terahertz range, the lower limit of the aforementioned distance is about 2 to about 3 μm.

In the waveguide device 100 of the above-described construction, a signal wave of the operating frequency is unable to propagate in the space between the surface 125 of the artificial magnetic conductor and the conductive surface 110 a of the conductive member 110, but propagates in the space between the waveguide surface 122 a of the waveguide member 122 and the conductive surface 110 a of the conductive member 110. Unlike in a hollow waveguide, the width of the waveguide member 122 in such a waveguide structure does not need to be equal to or greater than a half of the wavelength of the electromagnetic wave to propagate. Moreover, the conductive member 110 and the conductive member 120 do not need to be interconnected by a metal wall that extends along the thickness direction (i.e., in parallel to the YZ plane).

FIG. 5A schematically shows an electromagnetic wave that propagates in a narrow space, i.e., a gap between the waveguide surface 122 a of the waveguide member 122 and the conductive surface 110 a of the conductive member 110. Three arrows in FIG. 5A schematically indicate the orientation of an electric field of the propagating electromagnetic wave. The electric field of the propagating electromagnetic wave is perpendicular to the conductive surface 110 a of the conductive member 110 and to the waveguide surface 122 a.

On both sides of the waveguide member 122, stretches of artificial magnetic conductor that are created by the plurality of conductive rods 124 are present. An electromagnetic wave propagates in the gap between the waveguide surface 122 a of the waveguide member 122 and the conductive surface 110 a of the conductive member 110. FIG. 5A is schematic, and does not accurately represent the magnitude of an electromagnetic field to be actually created by the electromagnetic wave. A part of the electromagnetic wave (electromagnetic field) propagating in the space over the waveguide surface 122 a may have a lateral expanse, to the outside (i.e., toward where the artificial magnetic conductor exists) of the space that is delineated by the width of the waveguide surface 122 a. In this example, the electromagnetic wave propagates in a direction (i.e., the Y direction) which is perpendicular to the plane of FIG. 5A. As such, the waveguide member 122 does not need to extend linearly along the Y direction, but may include a bend(s) and/or a branching portion(s) not shown. Since the electromagnetic wave propagates along the waveguide surface 122 a of the waveguide member 122, the direction of propagation would change at a bend, whereas the direction of propagation would ramify into plural directions at a branching portion.

In the waveguide structure of FIG. 5A, no metal wall (electric wall), which would be indispensable to a hollow waveguide, exists on both sides of the propagating electromagnetic wave. Therefore, in the waveguide structure of this example, “a constraint due to a metal wall (electric wall)” is not included in the boundary conditions for the electromagnetic field mode to be created by the propagating electromagnetic wave, and the width (size along the X direction) of the waveguide surface 122 a is less than a half of the wavelength of the electromagnetic wave.

For reference, FIG. 5B schematically shows a cross section of a hollow waveguide 130. With arrows, FIG. 5B schematically shows the orientation of an electric field of an electromagnetic field mode (TE₁₀) that is created in the internal space 132 of the hollow waveguide 130. The lengths of the arrows correspond to electric field intensities. The width of the internal space 132 of the hollow waveguide 130 needs to be set to be broader than a half of the wavelength. In other words, the width of the internal space 132 of the hollow waveguide 130 cannot be set to be smaller than a half of the wavelength of the propagating electromagnetic wave.

FIG. 5C is a cross-sectional view showing an implementation where two waveguide members 122 are provided on the conductive member 120. Thus, an artificial magnetic conductor that is created by the plurality of conductive rods 124 exists between the two adjacent waveguide members 122. More accurately, stretches of artificial magnetic conductor created by the plurality of conductive rods 124 are present on both sides of each waveguide member 122, such that each waveguide member 122 is able to independently propagate an electromagnetic wave.

For reference's sake, FIG. 5D schematically shows a cross section of a waveguide device in which two hollow waveguides 130 are placed side-by-side. The two hollow waveguides 130 are electrically insulated from each other. Each space in which an electromagnetic wave is to propagate needs to be surrounded by a metal wall that defines the respective hollow waveguide 130. Therefore, the interval between the internal spaces 132 in which electromagnetic waves are to propagate cannot be made smaller than a total of the thicknesses of two metal walls. Usually, a total of the thicknesses of two metal walls is longer than a half of the wavelength of a propagating electromagnetic wave. Therefore, it is difficult for the interval between the hollow waveguides 130 (i.e., interval between their centers) to be shorter than the wavelength of a propagating electromagnetic wave. Particularly for electromagnetic waves of wavelengths in the extremely high frequency range (i.e., electromagnetic wave wavelength: 10 mm or less) or even shorter wavelengths, a metal wall which is sufficiently thin relative to the wavelength is difficult to be formed. This presents a cost problem in commercially practical implementation.

On the other hand, a waveguide device 100 including an artificial magnetic conductor can easily realize a structure in which waveguide members 122 are placed close to one another. Thus, such a waveguide device 100 can be suitably used in an array antenna that includes plural antenna elements in a close arrangement.

When a branching portion for branching the direction of propagation of a signal wave into two or more is introduced in a waveguide member 122 of the waveguide device as described above, unwanted reflection of the signal wave needs to be suppressed. This requires a higher degree of impedance matching at the branching portion. Structures for causing branching in a waveguide are used in transmission lines, such as microstrip lines, for example. When a branching portion is introduced in a transmission line such as a microstrip line, since a plurality of transmission lines exist beyond the branching portion, the impedance as viewed from before the branching portion will be a synthetic impedance of those of the plurality of transmission lines. Therefore, unless the characteristic impedances of the transmission lines are changed, a structure to convert impedance is often introduced in order to establish impedance matching before and after the branching portion. Such an impedance conversion structure is called an impedance transformer.

FIG. 6A is a diagram schematically showing an example of an impedance transformer which is used in a microstrip line. The arrows in the figure schematically indicate directions of propagation of signal waves. In a microstrip line, over a ¼ length of a wavelength λr of a signal wave in the waveguide, a portion which is broader in width than any adjacent site (which hereinafter may be referred to as a “broad portion”) is may be provided. The number of broad portions is not limited to one, and a plurality of broad portions of different widths may also be provided. The length of each broad portion along the direction of the line is λr/4, such that its width increases toward the branching portion. Such a structure is called a λ/4 transformer, which is used in order to establish impedance matching before and after a branching portion.

On the other hand, a branching portion having a T-shaped structure will result in a broader transmission line width; therefore, a notch is may be provided at a branching portion for width adjustment. FIG. 6B is a diagram schematically showing an exemplary structure of a branching portion in which such a notch is provided. An example of such a structure is disclosed in Kazuaki KAWABATA et al., “Computer Analysis of Microwave Planar Circuits by Finite Element Method: Right angle Corners and Tee Junctions”, Bulletin of the Faculty of Engineering, Hokkaido University, 77: 61-68, for example. By appropriately setting the shape and size of the notch, signal wave reflection can be suppressed.

A structure as shown in FIG. 6A and FIG. 6B might also be applied to the aforementioned ridge waveguide (WRG) in a similar manner. However, according to a study by the inventors, merely applying a structure as shown in FIG. 6A and FIG. 6B to a WRG will not sufficiently suppress signal wave reflection. Hereinafter, this problem will be described with reference to FIG. 7 through FIG. 11.

FIG. 7 and FIG. 8A are perspective views schematically showing part of the structure of a waveguide device according to comparative examples. FIG. 7 and FIG. 8A show part of a construction of the second conductive member 120, and a waveguide member 122 and a plurality of conductive rods 124 thereon. Upon these constituent elements, the aforementioned first conductive member 110 exists. The waveguide member 122 includes a first portion 122A extending along the Y direction, and a second portion 122B and a third portion 122C extending along the X direction. The first portion 122A, the second portion 122B, and the third portion 122C are connected at a branching portion 136 to constitute a T-shaped structure. In the following description, the first portion 122A may be referred to as a “stem”, whereas the second portion 122B and the third portion 122C may be referred to as “branches”. The first to third portions 122A to 122C will be collectively referred to as the “waveguide member 122”.

In the example of FIG. 8A, the width of the waveguide surface of the waveguide member 122 at the first portion 122A varies with distance from the branching portion 136 so as to present a staircase shape. Within the first portion 122A, each portion of identical width has a length along the Y direction which is ¼ of a wavelength λr of a signal wave in the waveguide. At any site, each portion of identical width has a length along the Y direction which is greater than the width of the waveguide surface. The width of the waveguide surface at the first portion 122A increases, in steps, toward the branching portion 136. Such a structure functions as the aforementioned λ/4 transformer (impedance transformer).

FIG. 8B is a diagram showing enlarged the structure near the branching portion 136 in FIG. 8A. The structure of this comparative example cannot sufficiently suppress signal wave reflection at the branching portion 136. The inventors infer that this is because capacitive coupling occurs on the inward of the branching portion 136 (i.e., between the stem 122A and the branch 122B, and between the stem 122A and the branch 122C) to result in excess capacitance components (parasitic capacitance). The arrows in FIG. 8B schematically indicate directions of electric fields between the stem 122A and the branches 122B and 122C. Owing to capacitance components occurring between the inward side surfaces of the branching portion 136, an electric field as shown in the figure may be created. In a WRG, it is considered that these capacitance components exert a nonnegligible influence on impedance matching. A similar problem also exists in the construction shown in FIG. 7. Thus, it has been found that adequate matching cannot be achieved even if a branching structure, which has been conventionally used in microstrip lines or the like, is applied to a WRG.

Generally speaking, in order to establish matching between a transmission line having an impedance Z₁ and a transmission line having an impedance Z₂, an impedance transformer having an impedance Z_(t) expressed as Z_(t)=(Z₁Z₂)^(1/2) may be introduced therebetween. For example, in a T-shaped waveguide in which the stem and the two branches all have an identical characteristic impedance, the impedance of the branching structure as viewed from the stem is ½ of the impedance of the stem (i.e., Z₂=Z₁/2). Therefore, in such a waveguide, matching can be achieved by setting the impedance of the impedance transformer to Z_(t)=Z₁/2^(1/2)(=Z₁/√ 2).

In order to reduce the characteristic impedance of a transmission line, its capacitance component C may be increased, or its inductance component L may be decreased. In a microstrip line, as described above, an impedance transformer is created by broadening the width of the waveguide. Also in a WRG, as in the example of FIG. 8A, the an impedance transformer can be created by broadening the width of the waveguide. However, as described earlier, the influence of parasitic capacitances occurring between the inward side surfaces of the branching portion 136 may make it difficult to achieve impedance matching. This problem is unique to a WRG, and has never been recognized in conventional transmission lines such as microstrip lines.

In a WRG, an effect which is similar or superior to increasing the width of the waveguide surface can be relatively easily achieved by reducing the distance between the waveguide surface 122 a of the waveguide member 122 and the conductive surface 110 a of the conductive member 110. The inventors have also studied such structures, but have concluded that, again, the influence of parasitic capacitance unique to a WRG must be taken into consideration.

FIG. 9A is a perspective view schematically showing part of the construction of a waveguide device structured so that the distance between the waveguide surface 122 a of the waveguide member 122 and the conductive surface 110 a of the conductive member 110 is decreased at impedance transformers. In this example, unlike in the example of FIG. 8A, not the width but the height of the waveguide surface 122 a of the waveguide member 122 at the first portion 122A is varied in steps. Similarly to varying the width, varying the height also provides an effect of increasing the capacitance between the waveguide surface 122 a and the conductive surface 110 a of the conductive member 110. Therefore, impedance adjustment is possible through adjusting the height of the waveguide member 122. Within the first portion 122A of the waveguide member 122, each portion of identical height has a length along the Y direction which is ¼ of a wavelength λr of a signal wave in the waveguide. Such a structure also functions as the aforementioned λ/4 transformer (impedance transformer).

Note that the length of each impedance transformer is not limited to ¼ of the wavelength λr of a signal wave in the waveguide. Under the influence of parasitic capacitance and the like associated with the WRG, the optimum length of an impedance transformer may vary around ¼ of λr. However, each impedance transformer has a length which is at least equal to the width of the waveguide surface 122 a, and yet does not exceed three times the width of the waveguide surface 122 a.

FIG. 9B is a diagram showing enlarged the construction near the branching portion 136 in FIG. 9A. In this comparative example, too, capacitive coupling occurs between the side surfaces of the first portion 122A of the waveguide member 122 and the side surfaces of the second and third portions 122B and 122C to result in excess capacitance components. Furthermore, in this comparative example, the elevated height of the first portion 122A in a region close to the branching portion 136 is also expected to create an excess capacitance component between the first portion 122A of the waveguide member 122 and the conductive surface 110 a of the first conductive member 110.

FIG. 10 is a diagram schematically showing a cross-sectional structure of the waveguide device in FIG. 9A as taken along a plane which passes through the first portion 122A of the waveguide member 122 and is parallel to the YZ plane. The arrows in FIG. 10 schematically indicate directions of an electric field. As shown in the figure, an impedance transformer 138 of the first portion 122A of the waveguide member 122 has a top surface which is more elevated from any adjacent site, and presumably for this reason, capacitive coupling occurs between its side surface or end face and the conductive surface 110 a of the conductive member 110. The inventors infer that a resultant capacitance component from this exerts a nonnegligible influence on impedance matching, similarly to the aforementioned capacitance components between the inward side surfaces of the branching portion 136.

FIG. 11 is a diagram showing an equivalent circuit of the waveguide structure in FIG. 9A. As mentioned above, at the branching portion 136, capacitive coupling occurs between the side surface of the first portion 122A of the waveguide member and the side surfaces of the second and third portions 122B and 122C. Consequently, excess capacitance components C1 are added to the existing inductance component L0, as shown in FIG. 11. Furthermore, capacitive coupling occurs between an upper portion of the side surface or end face of the leading end of the first portion 122A of the waveguide member 122 and the conductive surface 110 a of the conductive member 110. Consequently, an excess capacitance component C2 is added as shown in FIG. 11. These capacitance components C1 and C2 are considered to be one of the causes of the reduced degree of impedance matching at the branching portion 136.

Based on the above thoughts, as will be described in detail below, the inventors have succeeded in further enhancing the degree of impedance matching at a branching portion in a waveguide member, by improving the structure of the branching portion. The enhanced degree of impedance matching provides an improved propagation efficiency, and thus a waveguide device with less noise. It also becomes possible to enhance the performance of an antenna device that includes such a waveguide device. For example, establishment of impedance matching suppresses signal wave reflection, whereby power losses can be reduced, and a phase disturbance in the propagating electromagnetic wave can be suppressed. Therefore, in the context of communications, deteriorations in the communicated signals can be reduced, and in the context of radar, the accuracy of distance or direction-of-arrival estimation can be improved.

Hereinafter, more specific exemplary constructions for waveguide device and antenna devices according to example embodiments of the present disclosure will be described. Note however that unnecessarily detailed descriptions may be omitted. For example, detailed descriptions on what is well known in the art or redundant descriptions on what is substantially the same constitution may be omitted. This is to avoid lengthy description, and facilitate the understanding of those skilled in the art. The accompanying drawings and the following description, which are provided by the inventors so that those skilled in the art can sufficiently understand the present disclosure, are not intended to limit the scope of claims. In the present specification, identical or similar constituent elements are denoted by identical reference numerals.

<Waveguide Device>

Example Embodiment 1

FIG. 12A is a perspective view schematically showing part of the structure of a waveguide device according to Example Embodiment 1 of the present disclosure. FIG. 12B is an upper plan view showing the waveguide device of FIG. 12A as viewed from the +Z direction. FIG. 12C is a diagram showing the waveguide device of FIG. 12A as viewed from the +Y direction. FIGS. 12A through 12C only show a portion close to a branching portion 136 of a waveguide member 122 in illustrative manners. In actuality, the conductive member 120, the waveguide member 122, and plural conductive rods 124 may also exist in the surroundings of the portion that is shown in the figure. This waveguide device further includes a conductive member 110 (see FIG. 1, etc.) covering over the waveguide member 122 and the plurality of conductive rods 124. In the present specification, the conductive member 110 may be referred to as the “first conductive member”, and the conductive member 120 may be referred to as the “second conductive member” or a “further conductive member”.

The waveguide member 122 has: a waveguide surface 122 a opposing the conductive surface 110 a of the conductive member 110 and having a stripe shape (also referred to as a “strip shape”); and an electrically-conductive side surface 122 b that connects to the waveguide surface 122 a. In the present specification, a “stripe shape” means a shape which is defined by a single stripe, rather than a shape constituted by stripes. Not only shapes that extend linearly in one direction, but also any shape that bends or branches along the way is also encompassed by a “stripe shape”. In the case where any portion that undergoes a change in height or width is provided on the waveguide surface 122 a, it still falls under the meaning of “stripe shape” so long as the shape includes a portion that extends in one direction as viewed in the normal direction of the waveguide surface 122 a.

On both sides of the waveguide member 122, stretches of artificial magnetic conductor including a plurality of conductive rods 124 extend. The waveguide member 122 includes: a first portion 122A extending in one direction (which in the present example embodiment is the Y direction); and second and third portions 122B and 122C extending in mutually different directions (which in the present example embodiment are the +X direction and the −X direction) from one end of the first portion 122A. In the following description, the first portion 122A may be referred to as a “stem”, whereas the second and third portions 122B and 122C may each be referred to as a “branch”. In the present example embodiment, the waveguide member 122 includes two branches. The waveguide member 122 may include three or more branches. In other words, the waveguide member 122 may include at least two branches.

The waveguide member 122 according to the present example embodiment has a recess (or depression) 135 at the position of the branching portion 136. The gap between the waveguide surface 122 a of the waveguide member 122 and the conductive surface 110 a of the conductive member 110 is locally enlarged at the recess 135. Of a waveguide that is defined by the waveguide surface 122 a, the conductive surface 110 a, and the artificial magnetic conductor, any site presenting a locally enlarged gap will be referred to as a “gap enlargement”. At least a part of the branching portion 136, which is a junction where the first portion 122A of the waveguide member 122 becomes joined with the two branches (the second portion 122B and the third portion 122C), overlaps the gap enlargement as seen through in a direction perpendicular to the conductive surface 110 a.

As shown in FIG. 12C, given a width x of the recess 135 along the X direction and a difference z between the height of the waveguide surface 122 a from the root of the waveguide member 122 and the height of the bottom of the recess 135, x is greater than z. As will be described later in detail, the recess may alternatively be made in the conductive surface 110 a of the conductive member 110. FIG. 19 shows an exemplary structure in which a gap enlargement is realized by a recess 142 that is made in the conductive surface 110 a of the conductive member 110. In this structure, given a width x of the recess 142 along the X direction and a depth z of the bottom of the recess 142 relative to any site on the conductive surface 110 a that is adjacent to the recess 142, x is greater than z. In the case where recesses are made in both the waveguide surface 122 a and the conductive surface 110 a, z is a sum of the depth of the bottom of the recess in the waveguide surface 122 a relative to any site around the recess and the depth of the bottom of the recess in the conductive surface 110 a relative to any site around the recess.

Now, with reference to FIG. 12D and FIG. 12E, the junction (branching portion 136) according to the present example embodiment will be described. FIG. 12D is a view exclusively showing the waveguide member 122, out of the waveguide structure shown in FIG. 12B. FIG. 12E is a variant of the waveguide structure shown in FIG. 12D. The waveguide member 122 shown in FIG. 12E differs from the waveguide member 122 of FIG. 12D in that the first portion 122A intersects the second portion 122B and the third portion 122C at an angle which is not 90 degrees. Note that an implementation where the first portion 122A intersects either one of the second portion 122B and the third portion 122C at an angle which is not 90 degrees may also be a variant of the present example embodiment. The recess 135 is omitted from illustration in FIG. 12D and FIG. 12E. In the present disclosure, the junction (branching portion 136) is defined as, as illustrated in FIG. 12D and FIG. 12E, a region that is surrounded by imaginary extensions of an edge of the waveguide surface of the first portion, an edge of the waveguide surface of one branch, and an edge of the waveguide surface of the other branch. This region corresponds to the portion that is shown hatched in the figure. In FIG. 12B, the entire junction (branching portion 136) is located in a gap enlargement. In the case where there are three or more branches, a junction may also be similarly defined.

In the present example embodiment, the conductive surface 110 a opposing the waveguide surface 122 a is flat. Therefore, the position of the gap enlargement as seen through in a direction perpendicular to the conductive surface 110 a coincides with the position of the recess 135. In the case where the conductive surface 110 a is not flat, however, the position of the gap enlargement as seen through in a direction perpendicular to the conductive surface 110 a does not necessarily coincide with the position of the recess 135. Instead of or in addition to the recess 135 in the waveguide surface 122 a, a recess may be made in the conductive surface 110 a. So long as at least one of the waveguide surface 122 a and the conductive surface 110 a has a recess in the junction, a gap enlargement is created at that position.

In the present example embodiment, the dimension of the gap enlargement along the width direction of the first portion 122A of the waveguide member 122 is greater than the width of the first portion 122A. Herein, the width direction of the first portion 122A refers to the X direction, which is perpendicular to the Y direction (along which the first portion 122A extends). The dimension of the gap enlargement along the X direction may be equal to or less than the width of the first portion 122A.

In the present example embodiment, in the waveguide member 122, the first portion 122A intersects the second portion 122B and the third portion 122C at angles of substantially 90 degrees at the branching portion 136, thus constituting a T-shaped branching structure. The second portion 122B and the third portion 122C extend in mutually opposite directions from one end of the first portion 122A. The direction that the first portion 122A extends may not be orthogonal to the directions that the second and third portions 122B and 122C extend. Moreover, the second portion 122B and the third portion 122C may not extend in mutually opposite directions from one end of the first portion 122A. For example, a Y-shaped structure may be adopted such that bending by an angle which is greater than 90 degrees occurs from the first portion 122A of the waveguide member 122 to the second portion 122B and that bending by an angle which is greater than 90 degrees also occurs from the first portion 122A to the third portion 122C. The bending angle from the first portion 122A to the second portion 122B and the bending angle from the first portion 122A to the third portion 122C do not need to be equal. Moreover, although the example shown in FIG. 12A illustrates that the second portion 122B and the third portion 122C extend in mutually opposite directions from the branching portion 136, such a construction is not a limitation. The first portion 122A and the second portion 122B, or the first portion 122A and the third portion 122C, may extend in mutually opposite directions from the branching portion 136.

In the present example embodiment, the size of the gap between the waveguide surface 122 a and the conductive surface 110 a is greater at the gap enlargement than at any site on the waveguide that is adjacent to the gap enlargement, and is smaller than the distance between the conductive surface 110 a and a root 122D of the waveguide member 122. In the present example embodiment, the root 122D of the waveguide member 122 refers to the portion at which the waveguide member 122 and the conductive member 120 are connected; however, this structure is not limiting. In the case where the waveguide member 122 is not connected to the conductive member 120, as in a structure shown in FIG. 34B described later, the face of the waveguide member 122 that is opposed to the conductive member 120, i.e., the opposite face to the waveguide surface, may be referred to as the root of the waveguide member. In the present disclosure, the size of the gap of a gap enlargement means a maximum value of the size of the gap at that gap enlargement. For example, in the case where a bowl-shaped recess which exists in the waveguide surface 122 a constitutes a gap enlargement, the distance between the recess and the conductive surface at the deepest position of the bowl shape defines the size of the gap.

In the present example embodiment, an enhanced degree of impedance matching can be attained by providing a gap enlargement at the position of the branching portion 136. Hereinafter, this effect will be described.

FIG. 13 is a diagram showing an equivalent circuit of the ridge waveguide according to the present example embodiment. In the present example embodiment, the waveguide member 122 has a recess 135 in a region containing a branching portion 136. This structure is equivalent to a structure in which an inductance component L1 is added in parallel to a capacitance component C1 that is associated with the closeness between the electrically-conductive side surface of the stem of the waveguide member 122 and the electrically-conductive side surface of each of the two branches. This allows each capacitance component C1 occurring from bending at the branching portion 136 to be canceled with the inductance component L1. The magnitude of the inductance component L1 depends on the shape, size, and position of the recess 135. Therefore, the shape, size, and position of the recess 135 may be designed so that the inductance component L1 will cancel the unwanted capacitance component C1 at the branching portion 136.

With the above construction, the degree of impedance matching at the branching portion 136 is improved, whereby unwanted reflection of signal waves can be suppressed.

FIG. 14A and FIG. 14B are diagrams showing an implementation where an impedance matching structure is provided for the first portion 122A of the waveguide member 122. FIG. 14A shows an exemplary waveguide device having a staircase-shaped impedance matching structure, as in the comparative example shown in FIG. 9A. FIG. 14B shows an exemplary waveguide device having an impedance matching structure such that the width of the waveguide surface 122 a increases toward the branching portion 136, as in the comparative example shown in FIG. 8A.

An impedance transformer may be provided for at least one of: the waveguide surface 122 a of the first portion 122A; and the conductive surface 110 a opposing the waveguide surface 122 a of the first portion 122A. In the examples of FIG. 14A and FIG. 14B, two impedance transformers 138A and 138B are provided on the waveguide surface 122 a. Each impedance transformer allows the capacitance between the waveguide surface 122 a and the conductive surface 110 a to be increased relative to any adjacent site. In the example of FIG. 14A, each impedance transformer reduces the distance between the waveguide surface 122 a and the conductive surface 110 a relative to any adjacent site. In the example of FIG. 14B, each impedance transformer enlarges the width of the waveguide surface 122 a relative to any adjacent site. The length L of each of the impedance transformers 138A and 138B as measured along the direction that the first portion 122A extends (i.e., the Y direction) from an end of the first portion 122A adjoining the branching portion 136 is set to a value which is equal to or greater than the width of the waveguide surface 122 a.

FIG. 15A and FIG. 15B are diagrams showing other variants of the present example embodiment. In the example shown in FIG. 15A, the junction (branching portion 136) is contained in a recess 135 (gap enlargement) as seen through in a direction perpendicular to the conductive surface 110 a. In the example shown in FIG. 15B, the recess 135 as a rectangular-shape gap enlargement is provided in a central portion of the branching portion 136 of the waveguide member 122, without reaching the edge of any of the first portion 122A, the second portion 122B, or the third portion 122C. In other words, in the example of FIG. 15B, as seen through in a direction perpendicular to the conductive surface 110 a, the edge of the recess 135 (gap enlargement) is located inside the edge of the first portion 122A and the edges of the respective branches. In the variants shown in FIG. 15A and FIG. 15B, the wall surface of the recess 135 has a staircase shape. Such structures similarly provide impedance matching as do the above-described structures. Moreover, the recess 135 may be structured so that its wall surface is monotonically inclined toward the bottom of the recess 135.

FIG. 16A and FIG. 16B are diagrams showing still other variants. In the examples shown in FIG. 16A and FIG. 16B, at a junction where first to third portions 122A, 122B and 122C are joined with one another, the waveguide member 122 has a recess 139 reaching the waveguide surface 122 a (which may hereinafter be referred to as a “first recess”) on a side surface 122 s opposite to the first portion 122A. As viewed in a direction perpendicular to the waveguide surface 122 a or the conductive surface 110 a, the recess 139 overlaps the gap enlargement.

Adopting such structures further enhances the degree of impedance matching.

Hereinafter, with reference to FIG. 17A and FIG. 17B, it will be described how the construction according to the present example embodiment improves the degree of impedance matching at the branching portion 136 of the waveguide member 122.

The inventors have clarified through simulations that the construction according to the present example embodiment provides an improved degree of impedance matching as compared to the constructions of comparative examples (FIG. 7, FIG. 8A and FIG. 9A) where no gap enlargement exists in the branching portion. Herein, the degree of impedance matching is represented by an input reflection coefficient. An input reflection coefficient is a coefficient which represents a ratio of the intensity of a reflected wave to the intensity of an input wave, indicating the magnitude of return loss. It can be said that, the lower the input reflection coefficient is, the higher the degree of impedance matching is.

In this simulation, while setting various parameters to appropriate values, an input reflection coefficient S that resulted when an electromagnetic wave was propagated toward the branching portion 136 was measured as examples, regarding each of the construction of the comparative example shown in FIG. 9A and the construction of the example embodiment illustrated in FIG. 14A.

FIG. 17A and FIG. 17B are graphs showing results of this simulation. FIG. 17A shows frequency dependence of the input reflection coefficient (unit: dB) in the construction of the comparative example shown in FIG. 9A. FIG. 17B shows frequency dependence of the input reflection coefficient (unit: dB) in the example embodiment illustrated in FIG. 14A. As can be seen from FIG. 17A and FIG. 17B, at any frequency, the return loss is kept lower in the construction of FIG. 14A than in the construction of the comparative example. Moreover, in a broad frequency range from 67 GHz to 81 GHz, a relatively low return loss of −20 dB or less is realized. In UWB, for which a license is not a requisite, a bandwidth accounting for 5% of the used frequency is supposed to be required. It has been confirmed that the construction according to the present example embodiment achieves low losses across a bandwidth which is far greater than this bandwidth.

The above structure is likely to be easier to manufacture than is the structure disclosed in A. Uz. Zaman and P.-S. Kildal, “Ku Band Linear Slot-Array in Ridge Gapwaveguide Technology, EUCAP 2013, 7th European Conference on Antenna and Propagation. In A. Uz. Zaman and P.-S. Kildal, “Ku Band Linear Slot-Array in Ridge Gapwaveguide Technology, EUCAP 2013, 7th European Conference on Antenna and Propagation, in order to enhance the degree of impedance matching at a branching portion, the waveguide member is notched so that the width of its waveguide surface is locally narrowed. Such structure is commonplace in microstrip lines, and is introduced in A. Uz. Zaman and P.-S. Kildal, “Slot Antenna in Ridge Gap Waveguide Technology,” 6th European Conference on Antennas and Propagation, Prague, March, 2012 and the like. Since a microstrip line is a metal foil that is in tight contact with a substrate, forming a structure featuring a locally-narrowed microstrip line does not present much of a problem. On the other hand, when such structure is applied to the waveguide member of a WRG, since the waveguide member is going to be a ridge-shaped member with a height which is around ¼ of the wavelength, a site having an extremely narrowed width and a comparatively high height with respect to its width will locally emerge. Such a narrow-widthed site very often makes it difficult to obtain a stable shape in mass production utilizing casting, plastic working, injection molding, or other production processes. In the case of manufacture by cutting, cutting a narrow-widthed site out of a waveguide member often requires a cautious cutting.

The branching portion according to the present disclosure does not necessarily require narrowing of the width of the waveguide member. When the waveguide surface is to be recessed, the processing will be in the direction of lowering the height of the waveguide member, and thus the waveguide member can be easily formed. When a conductive surface is to be recessed, there is no need to alter the shape of the waveguide member, and all that is necessary is to cause the flat conductive surface to be recessed. In either case, the processing is easy, and mass production is facilitated in particular.

As necessary, a site featuring a locally-narrowed width of the waveguide member and a gap enlargement may be used in combination. Although made more difficult by the formation of a narrow-widthed portion, manufacture would still be possible.

Example Embodiment 2

FIG. 18A is a perspective view schematically showing part of the structure of a waveguide device according to Example Embodiment 2 of the present disclosure. FIG. 18B is an upper plan view showing the waveguide device of FIG. 18A as viewed along the Z direction. In the present example embodiment, the waveguide member 122 includes a second portion 122B, a third portion 122C, and a fourth portion 122D (each corresponding to a “branch”), which extend in respectively different directions from one end of the first portion 122A. That is, the waveguide member 122 has three branches. The second portion 122B and the third portion 122C extend from the branching portion 136 in directions that are 180 degrees apart (which in the present example embodiment are the +X direction and the −X direction). The first portion 122A and the fourth portion 122D extend from the branching portion 136 in mutually different directions (which in the present example embodiment are the +Y direction and the −Y direction). In the waveguide member 122, the first portion 122A and fourth portion 122D intersect the second portion 122B and third portion 122C at angles of 90 degrees in the branching portion 136, thus constituting a cross-shaped branching structure. Note that the angle constituted by the direction that the first and fourth portions 122A and 122D extend and the direction that the second and third portions 122B and 122C extend is not limited to 90 degrees. Moreover, the second and third portions 122B and 122C may not extend in mutually opposite directions from one end of the first portion 122A. Furthermore, the angle constituted by the fourth portion 122D and the first portion 122A is not limited to 180 degrees.

A recess 135 is made at the junction at which the first portion 122A, the second portion 122B, the third portion 122C, and the fourth portion 122D are joined with one another, i.e., the branching portion 136. Similarly to Example Embodiment 1, the recess 135 improves the degree of impedance matching at the branching portion 136.

According to the present example embodiment, a signal wave that has propagated along the first portion 122A branches out into three, and propagates thereafter. The recess 135 being provided at the branching portion suppresses signal wave reflection upon branching. The number of branches from the waveguide member 122 may be four or more. The direction that each branch extends may also be arbitrarily selected.

In the present example embodiment, impedance transformers similar to that shown in the example of FIG. 14A are provided for the first portion 122A; however, a construction from which impedance transformers are omitted may also be possible. Alternatively, impedance transformers of a construction similar to that of FIG. 14B may be provided. In the present disclosure, impedance transformers of the first portion 122A are not essential elements.

Example Embodiment 3

FIG. 19 is a perspective view schematically showing part of the structure of a waveguide device according to Example Embodiment 3 of the present disclosure. In FIG. 19, elements which are hidden by the conductive member 110 are indicated with dotted lines. In the present example embodiment, a gap enlargement is realized by a recess 142 made in the conductive surface 110 a of the conductive member 110. Moreover, when the waveguide device is seen through in a direction perpendicular to the conductive surface 110 a (the −Z direction), the region in which the recess 142 exists covers the entire junction (branching portion 136) of the waveguide member. In other words, as seen through in a direction perpendicular to any site on the conductive surface 110 a that is around the gap enlargement, the entire junction is located inside the gap enlargement. No recess is made in the waveguide surface 122 a of the waveguide member 122.

In the construction according to the present example embodiment, too, a gap enlargement is created in a position overlapping the branching portion 136. This allows less increase in capacitance at the branching portion, and improves the degree of impedance matching. In FIG. 19, the width along the X direction and the width along the Y direction of the recess 142 are respectively greater than the width along the X direction and the width along the Y direction of the junction 136 of the waveguide member. As a result, even if the relative positions of the first conductive member 110 and the second conductive member 120 are offset in a direction along the conductive surface 110 a, it is still easy to maintain a state where the recess 142 covers the entire junction 136. As a result, the degree of impedance matching can be stably improved.

In addition to the construction according to the present example embodiment, a recess may be made also in the branching portion 136 of the waveguide member 122. Moreover, an impedance matching structure as shown in FIG. 14A or FIG. 14B may be provided for the first portion 122A. With any such construction, the effect of impedance matching will be further improved.

Next, variants of Example Embodiments 1 to 3 will be described.

FIG. 20A is a perspective view schematically showing part of the structure of a waveguide device according to a variant of Example Embodiment 1. FIG. 20B is an upper plan view showing the waveguide device of FIG. 20A as viewed from the +Z direction. In this variant, the dimension of the recess 135 along the X direction is equal to the width of the first portion 122A. In other words, the dimension of the gap enlargement along the width direction of the first portion 122A is equal to the width of the first portion 122A. A structure where the dimension of the gap enlargement along the width direction of the first portion 122A is equal to the width of the first portion 122A is applicable to Example Embodiments 2 and 3 as well.

FIG. 21A is a perspective view schematically showing part of the structure of a waveguide device according to another variant of Example Embodiment 1. FIG. 21B is an upper plan view showing the waveguide device of FIG. 21A as viewed from the +Z direction. In this variant, the dimension of the recess 135 along the X direction is smaller than the width of the first portion 122A. In other words, the dimension of the gap enlargement along the width direction of the first portion 122A is smaller than the width of the first portion 122A. A structure where the dimension of the gap enlargement along the width direction of the first portion 122A is smaller than the width of the first portion 122A is applicable to Example Embodiments 2 and 3 as well.

The gap enlargement according to any of these variants has a smaller geometric area as seen through in the +Z direction than that of the gap enlargement according to the example embodiment shown in FIG. 12A. In the structure of FIG. 20A, as seen through from the +Z direction, the gap enlargement and the junction are identical in geometric area and shape. In the structure of FIG. 21A, as seen through from the +Z direction, the gap enlargement only accounts for a part of the junction. Therefore, as compared to the aforementioned example embodiment, these variants provide little effect of canceling the capacitance between the side surface of the first portion 122A and the side surfaces of the second and third portions 122B and 122C of the waveguide member 122. However, the degree of impedance matching is still improved as compared to any construction where a gap enlargement is not provided. In the case where such a small gap enlargement is provided, as in e.g. Example Embodiment 4 to be described later, it will be effective to provide a recess reaching the waveguide surface 122 a on a side surface of at least one of the second portion 122B and the third portion 122C, this side surface connecting to the first portion 122A. By providing such a recess near the branching portion 136, the degree of impedance matching can be further enhanced, as will be described later.

Example Embodiment 4

FIG. 22A is a perspective view schematically showing part of the structure of a waveguide device according to Example Embodiment 4 of the present disclosure. FIG. 22B is an upper plan view showing the waveguide device of FIG. 22A as viewed from the +Z direction. In the present example embodiment, the waveguide member 122 has two recesses (or depressions) 137 on side surfaces near the branching portion 136. Otherwise, its construction is similar to the construction shown in FIG. 14B.

FIG. 23A is an upper plan view showing enlarged only the waveguide member 122 in the structure shown in FIG. 22A. In the present example embodiment, each of the second portion 122B and the third portion 122C of the waveguide member 122 has a recess 137 on its side surface that connects to the first portion 122A. Each recess 137 has a semicylindrical shape extending along a direction (the Z direction) which is perpendicular to the waveguide surface 122 a, and reaches the waveguide surface 122 a (top surface). Because of the recesses 137, the distance between the side surface of the first portion 122A of the waveguide member and the side surfaces of the second portion 122B and the third portion 122C is increased, thereby suppressing unwanted capacitance components. Note that, without being limited to the shape shown, the recesses 137 may take a variety of shapes as will be described below. Although the present example embodiment illustrates that the two recesses 137 reach the root of the waveguide member 122 (i.e., the portion at which the waveguide member 122 and the second conductive member 120 are connected), one or both of these may not reach the root. The recesses 137 may be formed only in upper portions that are closer to the waveguide surface 122 a.

The waveguide device of the present example embodiment is used to propagate electromagnetic waves of a predetermined band that accommodates electromagnetic waves having a wavelength λo in free space. The predetermined band may be a band which is defined by a range of frequencies belonging to the millimeter waves (about 30 GHz to about 300 GHz), for example. The wavelength λo may be a wavelength (central wavelength) corresponding to the center frequency of such a band, for example. Given that an electromagnetic wave having a wavelength λo in free space has a wavelength λr when propagating in a waveguide extending between the conductive surface 110 a of the conductive member 110 and the waveguide surface 122 a of the waveguide member 122, the first portion 122A of the waveguide member 122 includes an impedance transformer 138A (which increases the capacitance of the waveguide) spanning a length of λr/4 from one end that is closer to the branching portion 136. The waveguide member 122 in the present example embodiment further includes another impedance transformer 138B spanning a length of λr/4 adjoining the impedance transformer 138A.

Each impedance transformer 138A, 138B in the present example embodiment is a broad portion of the waveguide member 122 that is greater in width than any adjacent site. The impedance transformer 138A, which is the closer one to the branching portion 136, has a greater width than the width of the other impedance transformer 138B.

Although the present example embodiment illustrates that the number of impedance transformers is two, there may be one, or three or more impedance transformer(s). Without being limited to a broad portion, each impedance transformer may be a protrusion which makes the distance between the conductive surface 110 a and the waveguide surface 122 a smaller at the waveguide member 122 than at any adjacent site. It suffices if each impedance transformer is greater in at least one of height and width than any adjacent site.

As shown in FIG. 23A, each of the two recesses 137 is provided near one end of the first portion 122A of the waveguide member 122. More specifically, as viewed from a direction which is perpendicular to the waveguide surface 122 a, the distance a from a point of intersection P between the side surface of the first portion 122A of the waveguide member 122 and the side surface of the second portion 122B to the center of the recess 137 along the X direction (i.e., the direction that the second portion 122B extends) is shorter than the length d of the recess 137 along this direction. The relationship between distance a and length d similarly applies to the recess 137 in the side surface of the third portion 122C of the waveguide member 122. In other words, as viewed from a direction which is perpendicular to the waveguide surface 122 a, the distance from a point of intersection between the side surface of the first portion 122A and the side surface of the third portion 122C to the center of the recess 137 in the third portion 122C is shorter than the length of the recess 137 along the direction that the third portion 122C extends.

Although the present example embodiment illustrates that the first portion 122A of the waveguide member 122 is continuous with an end of the recess 137 at the point P, this example is not a limitation. For instance, as shown in FIG. 23B, the end of the recess 137 may be remoted from the point of intersection P between the side surface of the first portion 122A of the waveguide member 122 and the side surface of the second portion 122B. The same also applies to the recess 137 in the third portion 122C. Also in this case, a sufficient effect can be achieved so long as a<d is satisfied.

In the present example embodiment, too, the number of branches is not limited to two. FIG. 24 is an upper plan view showing a waveguide device which includes a waveguide member 122 having three branches as viewed from the +Z direction. The waveguide member 122 includes a second portion 122B, a third portion 122C, and a fourth portion 122D (each corresponding to a “branch”), which extend in respectively different directions from one end of the first portion 122A. The second portion 122B and the third portion 122C extend from the branching portion 136 in directions that are 180 degrees apart (which in the present example embodiment are the +X direction and the −X direction). The first portion 122A and the fourth portion 122D extend from the branching portion 136 in mutually different directions (which in the present example embodiment are the +Y direction and the −Y direction). In the waveguide member 122, the first portion 122A and fourth portion 122D intersect the second portion 122B and third portion 122C at angles of 90 degrees in the branching portion 136, thus constituting a cross-shaped branching structure. Note that the angle constituted by the direction that the first and fourth portions 122A and 122D extend and the direction that the second and third portions 122B and 122C extend is not limited to 90 degrees. Moreover, the second and third portions 122B and 122C may not extend in mutually opposite directions from one end of the first portion 122A. Furthermore, the angle constituted by the fourth portion 122D and the first portion 122A is not limited to 180 degrees.

In the present example embodiment, the waveguide member 122 has a recess 137 in each of: a site at which a side surface of the first portion 122A meets a side surface of the second portion 122B; and a site at which a side surface of the first portion 122A meets a side surface of the third portion 122C. Moreover, the waveguide member 122 has a recess 137 in each of: a site at which a side surface of the fourth portion 122D meets a side surface of the second portion 122B; and a site at which a side surface of the fourth portion 122D meets a side surface of the third portion 122C. Each recess 137 extends along a direction (the Z direction) which is perpendicular to the waveguide surface 122 a, and reaches the waveguide surface 122 a (top surface). Moreover, each recess 137 has a circular arc shape in a cross section that is perpendicular to the Z direction (which may hereinafter be referred to as a “horizontal cross section”). The shape of each recess 137 in a horizontal cross section may be different from a circular arc shape, e.g., a combination of a circular arc and straight lines extending from the ends of the circular arc. Thus, a horizontal cross section of each recess 137 may have a variety of shapes.

Thus, in the present example embodiment, each of the second portion 122B and the third portion 122C of the waveguide member 122 has a recess 137 at its side surface closer to the impedance transformer 138A in the first portion 122A, the recesses 137 reaching the waveguide surface 122 a. This structure is equivalent to a structure where an inductance component L1 is added in parallel to each capacitance component C1 that is associated with the closeness between electrically-conductive side surfaces at the branching portion 136. Therefore, although the ridge waveguide shown in FIG. 22A has an equivalent circuit construction which is similar to the equivalent circuit shown in FIG. 13, the added inductance component L1 is even greater. This makes it even easier to cancel with the inductance component L1 each capacitance component C1 occurring from bending at the branching portion 136. The magnitude of the added inductance component L1 depends on the shape, size, and position of each recess 137. Therefore, the shape, size, and position of each recess 137 may be designed so that the inductance component L1 will cancel the unwanted capacitance component C1 at the branching portion 136. Although the construction of FIG. 22A is discussed herein, similar effects will also be obtained in constructions other than that of FIG. 22A.

FIG. 25A is a perspective view showing part of the structure of a waveguide device according to still another variant of the present example embodiment. FIG. 25B is an upper plan view showing the structure of FIG. 25A as viewed from the +Z direction. In the present example embodiment, the two impedance transformers 138A and 138B in the first portion 122A of the waveguide member 122 are realized by a structure with varying height, rather than width, of the waveguide surface 122 a. Such structure also provides similar effects.

With the above construction, the degree of impedance matching at the branching portion 136 is improved, and unwanted reflection of signal waves can be suppressed.

Example Embodiment 5

FIG. 26A is a perspective view showing part of the structure of a waveguide device according to Example Embodiment 5 of the present disclosure. FIG. 26B is an upper plan view showing the structure of FIG. 26A as viewed from the +Z direction. In the present example embodiment, the two impedance transformers 138A and 138B in the first portion 122A of the waveguide member 122 are realized by a structure with varying height, rather than width, of the waveguide surface 122 a. Moreover, on a side surface opposite from the first portion 122A, the waveguide member 122 has a recess 139 at the junction (branching portion 136) where the first to third portions 122A to 122C are joined with one another, the recess 139 reaching the waveguide surface 122 a. In the present specification, the recess 139 in the branching portion 136 may be referred to as a “first recess”, the recess 137 in the second portion 122B as a “second recess”, and the recess 137 in the third portion 122C as a “third recess”. Similarly to the first and second recesses 137, the third recess 139 may or may not reach the root of the waveguide member 122.

FIG. 27 is a perspective view showing enlarged only a portion of the waveguide member 122 for ease of understanding. As shown in the figure, in the present example embodiment, the height of the waveguide surface 122 a at the impedance transformer 138A is greater than the height of the waveguide surface 122 a at the second portion 122B and third portion 122C. Therefore, capacitive coupling occurs between the side surface 138 a of the impedance transformer 138A and the conductive surface 110 a of the conductive member 110, whereby an unwanted capacitance component C2 occurs in the waveguide (see FIG. 11). In the present example embodiment, providing the third recess 139 reduces this unwanted capacitance component C2. Note that the impedance transformers 138A and 138B may be provided on the conductive member 110 facing the waveguide surface 122 a, or provided both on the waveguide surface 122 a and on the conductive member 110. Such examples will be described later with reference to FIG. 29A and FIG. 29B.

FIG. 28 is a diagram showing an equivalent circuit of the ridge waveguide according to the present example embodiment. A structure having the third recess 139 is equivalent to a structure where an inductance component L2 is added in parallel to the capacitance component C2. By providing the recess 139 in addition to the recess 135 and the two recesses 137, not only the capacitance components C1 associated with bending at the branching portion 136, but also the capacitance component C2 associated with the impedance transformer 138A can be canceled. The magnitude of the added inductance component L2 depends on the shape, size, and position of the third recess 139. Therefore, the shape, size, and position of the third recess 139 may be designed so that the inductance components L1 and L2 will cancel the capacitance components C1 and C2.

With such a construction, impedance matching is established at the branching portion 136 and signal wave reflection can be suppressed, whereby a decrease in transmission efficiency can be reduced.

In the present example embodiment, inductance components can be added to the branching portion 136 in two ways, thereby making it so much easier to establish matching. In particular, this facilitates matching across a broad frequency band, which will be required in the case of handling radio waves of the UWB (Ultra Wide Band), for which a license is not a requisite.

Other Example Embodiments

The waveguide device according to the present disclosure permits various modifications, without being limited to the above example embodiments. Hereinafter, other example embodiments of the waveguide device will be described.

In Example Embodiments 4 and 5, recesses 137 are made in side surfaces of both of the second portion 122B and the third portion 122C of the waveguide member 122; alternatively, a recess 137 may be made in a side surface of either one of them. Such a construction will particularly find its use in the cases where an angle constituted by the direction that the first portion 122A of the waveguide member 122 extends and the direction that the second portion 122B extends is different from an angle constituted by the direction that the first portion 122A extends and the direction that the third portion 122C extends.

FIG. 29A and FIG. 29B are cross-sectional views schematically showing other examples of the impedance transformer 138. In the example shown in FIG. 29A, protrusions function as impedance transformers 138 are formed on the conductive surface 110 a of the conductive member 110. On the other hand, in the example shown in FIG. 29B, structures functioning as impedance transformers 138 are formed on both of the conductive surface 110 a and the waveguide surface 122 a. In the example of FIG. 29B, neither the waveguide member 122 nor the conductive member 110 has a structure with a length of λr/4 per se along the Y direction, but in combination, they define a region with a length of λr/4 with a smaller gap than at any adjacent site. In the present disclosure, such a structure also qualifies as an impedance transformer 138. As in these examples, the impedance transformer 138 may be formed on at least one of: the waveguide surface 122 a of the waveguide member 122 at the first portion 122A; and the conductive surface 110 a opposing the waveguide surface 122 a. Each impedance transformer 138 spans a length of λr/4 along the Y direction from one end of the first portion 122A. In the examples shown in FIG. 29A and FIG. 29B, each impedance transformer 138 is a portion with a smaller gap size between the waveguide surface 122 a and the conductive surface 110 a than in any adjacent site, and includes at least a portion of a protrusion on at least one of the waveguide surface 122 a and the conductive surface 110 a.

As described earlier, the length of each impedance transformer 138 along the Y direction is not limited to λr/4. Under the influence of parasitic capacitance and the like associated with the WRG, an optimum length of an impedance transformer 138 may vary from λr/4. The length of each impedance transformer 138 along the waveguide surface 122 a may be equal to or greater than the width of the waveguide surface 122 a and less than three times the width of the waveguide surface 122 a, for example. Note that the width of the waveguide surface 122 a may vary with position, as in Example Embodiment 2. In that case, the “width” of the waveguide surface 122 a means the width of the broadest portion of the waveguide surface 122 a.

Next, with reference to FIGS. 30A through 30D, other exemplary gap enlargements according to example embodiments of the present disclosure will be described.

FIG. 30A shows an example where, as viewed in a direction perpendicular to the conductive surface 110 a, the dimension of a gap enlargement 141 along the width direction of the first portion 122A of the waveguide member decreases toward the first portion 122A. In this example, as seen through in a direction perpendicular to any site on the conductive surface that is around the gap enlargement 141, the outer edge of the gap enlargement reaches an edge 143 of the two branches 122B and 122C or the junction on the opposite side from the first portion 122A, but does not reach two edges 145 of the first portion 122A.

FIG. 30B shows an example where, as viewed in a direction perpendicular to the conductive surface 110 a, the dimension of a gap enlargement 141 along the width direction of the first portion 122A of the waveguide member increases toward the first portion 122A. In this example, as seen through in a direction perpendicular to any site on the conductive surface that is around the gap enlargement 141, the outer edge of the gap enlargement reaches an edge 143 of the two branches 122B and 122C or the junction on the opposite side from the first portion 122A, and also reaches two edges 145 of the first portion 122A.

In the examples shown in FIG. 30A and FIG. 30B, the shape of the gap enlargement as viewed in a direction perpendicular to the conductive surface 110 a is a trapezoid, rather than a rectangle.

FIG. 30C shows an example where a gap enlargement 141 of an elliptic shape is provided in a central portion of a branching portion of the waveguide member, without reaching the edge of any of the first portion 122A, the second portion 122B, or the third portion 122C. FIG. 30D shows an example where a gap enlargement 141 of a semicircular shape is located adjacent to an end of the first portion 122A of the waveguide member. In these constructions, too, effects of the example embodiments of the present disclosure can be obtained.

The side walls of junction between the first portion and each branch of the waveguide member may be rounded. In other words, the side-surface junction between the side surface of the first portion and the side surface(s) of at least one of the second and third portions of the waveguide member may be curved. For example, as shown in FIG. 31A, the side surface of the first portion 122A and the side surfaces of the second portion 122B and the third portion 122C may present curved connection. Furthermore, as shown in FIG. 31B, the side surface of the fourth portion 122D and the side surfaces of the second portion 122B and the third portion 122C may also present curved connection.

Thus, a waveguide device according to an example embodiment of the present disclosure includes: a conductive member 110 having a conductive surface 110 a; a waveguide member 122 having an electrically-conductive waveguide surface 122 a which is opposed to the conductive surface 110 a and an electrically-conductive side surface which is connected to the waveguide surface 122 a, and extending alongside the conductive surface 110 a; and an artificial magnetic conductor extending on both sides of the waveguide member 122. The waveguide member 122 includes: a first portion 122A extending in one direction; and at least two branches extending from one end of the first portion 122A, the at least two branches including a second portion 122B and a third portion 122C that extend in mutually different directions. A waveguide which is defined by the conductive surface 110 a, the waveguide surface 122 a, and the artificial magnetic conductor includes a gap enlargement at which a gap between the conductive surface 110 a and the waveguide surface 122 a is locally enlarged. At least a part of a junction at which the first portion 122A of the waveguide member 122 becomes jointed with the at least two branches overlaps the gap enlargement, as seen through in a direction perpendicular to the conductive surface 110 a. With such construction, the degree of impedance matching at any branching portion can be enhanced.

<Antenna Device>

Next, an illustrative example embodiment of an antenna device including the waveguide device according to the present disclosure will be described.

An antenna device according to the present example embodiment includes a waveguide device according to any of the above example embodiments and at least one antenna element connected to the waveguide device. The antenna element has at least one of the function of radiating into space an electromagnetic wave which has propagated through a waveguide in the waveguide device and the function of allowing an electromagnetic wave which has propagated in space to be introduced into a waveguide in the waveguide device. In other words, the antenna device according to the present example embodiment is used for at least one of transmission and reception of signals.

FIG. 32A is an upper plan view of an antenna device (array antenna) including 16 slots (openings) 112 in an array of 4 rows and 4 columns, as viewed from the Z direction. FIG. 32B is a cross-sectional view taken along line B-B in FIG. 32A. In the antenna device shown in the figures, a first waveguide device 100 a and a second waveguide device 100 b are layered. The first waveguide device 100 a includes waveguide members 122U that directly couple to slots 112 functioning as radiation elements (antenna elements). The second waveguide device 100 b includes further waveguide members 122L that couple to the waveguide members 122U of the first waveguide device 100 a. The waveguide members 122L and the conductive rods 124L of the second waveguide device 100 b are arranged on a third conductive member 140. The second waveguide device 100 b is basically similar in construction to the first waveguide device 100 a.

On the first conductive member 110 in the first waveguide device 100 a, side walls 114 surrounding each slot 112 are provided. The side walls 114 form a horn that adjusts directivity of the slot 112. The number and arrangement of slots 112 in this example are only illustrative. The orientations and shapes of the slots 112 are not limited to those of the example shown in the figures, either. It is not intended that the example shown in the figures provides any limitation as to whether the side walls 114 of each horn are tilted or not, the angles thereof, or the shape of each horn.

FIG. 33A is a diagram showing a planar layout of waveguide members 122U in the first waveguide device 100 a. FIG. 33B is a diagram showing a planar layout of a waveguide member 122L in the second waveguide device 100 b. As is clear from these figures, the waveguide members 122U of the first waveguide device 100 a extend linearly, and include no branching portions or bends. On the other hand, the waveguide members 122L of the second waveguide device 100 b include both branching portions and bends. In terms of fundamental construction of the waveguide device, the combination of the “second conductive member 120” and the “third conductive member 140” in the second waveguide device 100 b corresponds to the combination in the first waveguide device 100 a of the “first conductive member 110” and the “second conductive member 120”.

What is characteristic in the array antenna shown in the figures is that recesses 135 are respectively formed in three branching portions 136 of the waveguide member 122L. As a result, the degree of impedance matching is improved at the branching portions 136 of the waveguide members 122L.

The waveguide members 122U of the first waveguide device 100 a couple to the waveguide member 122L of the second waveguide device 100 b, through ports (openings) 145U that are provided in the second conductive member 120. Stated otherwise, an electromagnetic wave which has propagated through the waveguide member 122L of the second waveguide device 100 b passes through a port 145U to reach a waveguide member 122U of the first waveguide device 100 a, and propagates through the waveguide member 122U of the first waveguide device 100 a. In this case, each slot 112 functions as an antenna element to allow an electromagnetic wave which has propagated through the waveguide to be emitted into space. Conversely, when an electromagnetic wave which has propagated in space impinges on a slot 112, the electromagnetic wave couples to the waveguide member 122U of the first waveguide device 100 a that lies directly under that slot 112, and propagates through the waveguide member 122U of the first waveguide device 100 a. An electromagnetic wave which has propagated through a waveguide member 122U of the first waveguide device 100 a may also pass through a port 145U to reach the waveguide member 122L of the second waveguide device 100 b, and propagates through the waveguide member 122L of the second waveguide device 100 b. Via a port 145L of the third conductive member 140, the waveguide member 122L of the second waveguide device 100 b may couple to an external waveguide device or radio frequency circuit (electronic circuit).

As one example, FIG. 33B illustrates an electronic circuit 200 which is connected to the port 145L. Without being limited to a specific position, the electronic circuit 200 may be provided at any arbitrary position. The electronic circuit 200 may be provided on a circuit board which is on the rear surface side (i.e., the lower side in FIG. 32B) of the third conductive member 140, for example. Such an electronic circuit is a microwave integrated circuit, which may be an MMIC (Monolithic Microwave Integrated Circuit) that generates or receives millimeter waves, for example.

The first conductive member 110 shown in FIG. 32A may be called an “emission layer”. Moreover, the entirety of the second conductive member 120, the waveguide members 122U, and the conductive rods 124U shown in FIG. 33A may be called an “excitation layer”, whereas the entirety of the third conductive member 140, the waveguide member 122L, and the conductive rods 124L shown in FIG. 33B may be called a “distribution layer”. Moreover, the “excitation layer” and the “distribution layer” may be collectively called a “feeding layer”. Each of the “emission layer”, the “excitation layer”, and the “distribution layer” can be mass-produced by processing a single metal plate. The radiation layer, the excitation layer, the distribution layer, and the electronic circuitry to be provided on the rear face side of the distribution layer may be fabricated as a single-module product.

In the array antenna of this example, as can be seen from FIG. 32B, an emission layer, an excitation layer, and a distribution layer are layered, which are in plate form; therefore, a flat and low-profile flat panel antenna is realized as a whole. For example, the height (thickness) of a multilayer structure having a cross-sectional construction as shown in FIG. 32B can be set to 10 mm or less.

With the waveguide member 122L shown in FIG. 33B, the distances from the port 145L of the third conductive member 140 to the respective ports 145U (see FIG. 33A) of the second conductive member 120 measured along the waveguide member 122L are all equal. Therefore, a signal wave which is input to the waveguide member 122L reaches the four ports 145U of the second conductive member 120 all in the same phase, from the port 145L of the third conductive member 140. As a result, the four waveguide members 122U on the second conductive member 120 can be excited in the same phase.

It is not necessary for all slots 112 functioning as antenna elements to emit electromagnetic waves in the same phase. The network patterns of the waveguide members 122U and 122L in the excitation layer and the distribution layer may be arbitrary, and they may be arranged so that the respective waveguide members 122U and 122L independently propagate different signals.

Although the waveguide members 122U of the first waveguide device 100 a in this example include neither a branching portion nor a bend, the waveguide device functioning as an excitation layer may also include a waveguide member having at least one of a branching portion and a bend. In the example shown in FIG. 33A, each port 145U is located at the central portion of the waveguide member 122U. By placing the port 145U at the central portion of the waveguide member 122U, the distance from the port 145U to the slot 112 located at the end of the waveguide member 122U can be shortened. Shortening this distance will reduce the phase differences at each slot 112 to occur when the frequency of the electromagnetic wave is varied, thereby making it possible to excite the slots 112 under appropriate phase conditions over a broader band.

<Other Variants>

Next, variants of waveguide structures including the waveguide member 122, the conductive members 110 and 120, and the plurality of conductive rods 124 will be described. The following variants are applicable to the WRG structure in any place in each of the example embodiments described above.

FIG. 34A is a cross-sectional view showing an exemplary structure in which only the waveguide surface 122 a, defining an upper face of the waveguide member 122, is electrically conductive, while any portion of the waveguide member 122 other than the waveguide surface 122 a is not electrically conductive. Both of the conductive member 110 and the conductive member 120 alike are only electrically conductive at their surface that has the waveguide member 122 provided thereon (i.e., the conductive surface 110 a, 120 a), while not being electrically conductive in any other portions. Thus, each of the waveguide member 122, the conductive member 110, and the conductive member 120 does not need to be electrically conductive.

FIG. 34B is a diagram showing a variant in which the waveguide member 122 is not formed on the conductive member 120. In this example, the waveguide member 122 is fixed to a supporting member (e.g., the inner wall of the housing) that supports the conductive member 110 and the conductive member. A gap exists between the waveguide member 122 and the conductive member 120. Thus, the waveguide member 122 does not need to be connected to the conductive member 120.

FIG. 34C is a diagram showing an exemplary structure where the conductive member 120, the waveguide member 122, and each of the plurality of conductive rods 124 are composed of a dielectric surface that is coated with an electrically conductive material such as a metal. The conductive member 120, the waveguide member 122, and the plurality of conductive rods 124 are connected to one another via the electrical conductor. On the other hand, the conductive member 110 is made of an electrically conductive material such as a metal.

FIG. 34D and FIG. 34E are diagrams each showing an exemplary structure in which dielectric layers 110 c and 120 c are respectively provided on the outermost surfaces of conductive members 110 and 120, a waveguide member 122, and conductive rods 124. FIG. 34D shows an exemplary structure in which the surface of metal conductive members, which are electrical conductors, are covered with a dielectric layer. FIG. 34E shows an example where the conductive member 120 is structured so that the surface of members which are composed of a dielectric, e.g., resin, is covered with an electrical conductor such as a metal, this metal layer being further coated with a dielectric layer. The dielectric layer that covers the metal surface may be a coating of resin or the like, or an oxide film of passivation coating or the like which is generated as the metal becomes oxidized.

The dielectric layer on the outermost surface will allow losses to be increased in the electromagnetic wave propagating through the WRG waveguide, but is able to protect the conductive surfaces 110 a and 120 a (which are electrically conductive) from corrosion. It also prevents influences of a DC voltage, or an AC voltage of such a low frequency that it is not capable of propagation on certain WRG waveguides.

FIG. 34F is a diagram showing an example where the height of the waveguide member 122 is lower than the height of the conductive rods 124, and the portion of the conductive surface 110 a of the conductive member 110 that opposes the waveguide surface 122 a protrudes toward the waveguide member 122. Even such a structure will operate in a similar manner to the above-described example embodiment, so long as the ranges of dimensions depicted in FIG. 4 are satisfied.

FIG. 34G is a diagram showing an example where, further in the structure of FIG. 34F, portions of the conductive surface 110 a that oppose the conductive rods 124 protrude toward the conductive rods 124. Even such a structure will operate in a similar manner to the above-described example embodiment, so long as the ranges of dimensions depicted in FIG. 4 are satisfied. Instead of a structure in which the conductive surface 110 a partially protrudes, a structure in which the conductive surface 110 a is partially dented may be adopted.

FIG. 35A is a diagram showing an example where a conductive surface 110 a of the conductive member 110 is shaped as a curved surface. FIG. 35B is a diagram showing an example where also a conductive surface 120 a of the conductive member 120 is shaped as a curved surface. As demonstrated by these examples, the conductive surfaces 110 a and 120 a may not be shaped as planes, but may be shaped as curved surfaces. A conductive member having a conductive surface which is a curved surface is also qualifies as a conductive member having a “plate shape”.

In the waveguide device 100 of the above-described construction, a signal wave of the operating frequency is unable to propagate in the space between the surface 125 of the artificial magnetic conductor and the conductive surface 110 a of the conductive member 110, but propagates in the space between the waveguide surface 122 a of the waveguide member 122 and the conductive surface 110 a of the conductive member 110. Unlike in a hollow waveguide, the width of the waveguide member 122 in such a waveguide structure does not need to be equal to or greater than a half of the wavelength of the electromagnetic wave to propagate. Moreover, the conductive member 110 and the conductive member 120 do not need to be electrically interconnected by a metal wall that extends along the thickness direction (i.e., in parallel to the YZ plane).

An antenna device (slot array antenna) according to an example embodiment of the present disclosure can be suitably used in a radar device or a radar system to be incorporated in moving entities such as vehicles, marine vessels, aircraft, robots, or the like, for example. A radar device would include a slot array antenna according to an example embodiment of the present disclosure and a microwave integrated circuit that is connected to the slot array antenna. A radar system would include the radar device and a signal processing circuit that is connected to the microwave integrated circuit of the radar device. An antenna device according to an example embodiment of the present disclosure includes a multi-layered WRG structure which permits downsizing, and thus allows the area of the face on which antenna elements are arrayed to be significantly reduced, as compared to a construction in which a conventional hollow waveguide is used. Therefore, a radar system incorporating the antenna device can be easily mounted in a narrow place such as a face of a rearview mirror in a vehicle that is opposite to its specular surface, or a small-sized moving entity such as a UAV (an Unmanned Aerial Vehicle, a so-called drone). Note that, without being limited to the implementation where it is mounted in a vehicle, a radar system may be used while being fixed on the road or a building, for example.

A slot array antenna according to an example embodiment of the present disclosure can also be used in a wireless communication system. Such a wireless communication system would include a slot array antenna according to any of the above example embodiments and a communication circuit (a transmission circuit or a reception circuit). Details of exemplary applications to wireless communication systems will be described later.

A slot array antenna according to an example embodiment of the present disclosure can further be used as an antenna in an indoor positioning system (IPS). An indoor positioning system is able to identify the position of a moving entity, such as a person or an automated guided vehicle (AGV), that is in a building. A slot array antenna can also be used as a radio wave transmitter (beacon) for use in a system which provides information to an information terminal device (e.g., a smartphone) that is carried by a person who has visited a store or any other facility. In such a system, once every several seconds, a beacon may radiate an electromagnetic wave carrying an ID or other information superposed thereon, for example. When the information terminal device receives this electromagnetic wave, the information terminal device transmits the received information to a remote server computer via telecommunication lines. Based on the information that has been received from the information terminal device, the server computer identifies the position of that information terminal device, and provides information which is associated with that position (e.g., product information or a coupon) to the information terminal device.

The present specification employs the term “artificial magnetic conductor” in describing the technique according to the present disclosure, this being in line with what is set forth in a paper by one of the inventors Kirino (H. Kirino and K. Ogawa, “A 76 GHz Multi-Layered Phased Array Antenna using a Non-Metal Contact Metamaterial Wavegude”, IEEE Transaction on Antenna and Propagation, Vol. 60, No. 2, pp. 840-853, February, 2012) as well as a paper by Kildal et al., who published a study directed to related subject matter around the same time. However, it has been found through a study by the inventors that the invention according to the present disclosure does not necessarily require an “artificial magnetic conductor” under its conventional definition. That is, while a periodic structure has been believed to be a requirement for an artificial magnetic conductor, the invention according to the present disclosure does not necessary require a periodic structure in order to be practiced.

The artificial magnetic conductor that is described in the present disclosure consists of rows of conductive rods. Therefore, in order to prevent electromagnetic waves from leaking away from the waveguide surface, it has been believed essential that there exist at least two rows of conductive rods on one side of the waveguide member(s), such rows of conductive rods extending along the waveguide member(s) (ridge(s)). The reason is that it takes at least two rows of conductive rods for them to have a “period”. However, according to a study by the inventors, even when only one row of conductive rods exists between two waveguide members that extend in parallel to each other, the intensity of a signal that leaks from one waveguide member to the other waveguide member can be suppressed to −10 dB or less, which is a practically sufficient value in many applications. The reason why such a sufficient level of separation is achieved with only an imperfect periodic structure is so far unclear. However, in view of this fact, in the present disclosure, the notion of “artificial magnetic conductor” is extended so that the term also encompasses a structure including only one row of conductive rods.

Application Example 1: Onboard Radar System

Next, as an Application Example of utilizing the above-described slot array antenna, an instance of an onboard radar system including a slot array antenna will be described. A transmission wave used in an onboard radar system may have a frequency of e.g. 76 gigahertz (GHz) band, which will have a wavelength λo of about 4 mm in free space.

In safety technology of automobiles, e.g., collision avoidance systems or automated driving, it is particularly essential to identify one or more vehicles (targets) that are traveling ahead of the driver's vehicle. As a method of identifying vehicles, techniques of estimating the directions of arriving waves by using a radar system have been under development.

FIG. 36 shows a driver's vehicle 500, and a preceding vehicle 502 that is traveling in the same lane as the driver's vehicle 500. The driver's vehicle 500 includes an onboard radar system which incorporates a slot array antenna according to any of the above-described example embodiments. When the onboard radar system of the driver's vehicle 500 radiates a radio frequency transmission signal, the transmission signal reaches the preceding vehicle 502 and is reflected therefrom, so that a part of the signal returns to the driver's vehicle 500. The onboard radar system receives this signal to calculate a position of the preceding vehicle 502, a distance (“range”) to the preceding vehicle 502, velocity, etc.

FIG. 37 shows the onboard radar system 510 of the driver's vehicle 500. The onboard radar system 510 is provided within the vehicle. More specifically, the onboard radar system 510 is disposed on a face of the rearview mirror that is opposite to its specular surface. From within the vehicle, the onboard radar system 510 radiates a radio frequency transmission signal in the direction of travel of the vehicle 500, and receives a signal(s) which arrives from the direction of travel.

The onboard radar system 510 of this Application Example includes a slot array antenna according to an example embodiment of the present disclosure. The slot array antenna may include a plurality of waveguide members that are parallel to one another. They are to be arranged so that the plurality of waveguide members each extend in a direction which coincides with the vertical direction, and that the plurality of waveguide members are arranged in a direction which coincides with the horizontal direction. As a result, the lateral and vertical dimensions of the plurality of slots as viewed from the front can be further reduced.

Exemplary dimensions of an antenna device including the above array antenna may be 60 mm (wide)×30 mm (long)×10 mm (deep). It will be appreciated that this is a very small size for a millimeter wave radar system of the 76 GHz band.

Note that many a conventional onboard radar system is provided outside the vehicle, e.g., at the tip of the front nose. The reason is that the onboard radar system is relatively large in size, and thus is difficult to be provided within the vehicle as in the present disclosure. The onboard radar system 510 of this Application Example may be installed within the vehicle as described above, but may instead be mounted at the tip of the front nose. Since the footprint of the onboard radar system on the front nose is reduced, other parts can be more easily placed.

The Application Example allows the interval between a plurality of waveguide members (ridges) that are used in the transmission antenna to be narrow, which also narrows the interval between a plurality of slots to be provided opposite from a number of adjacent waveguide members. This reduces the influences of grating lobes. For example, when the interval between the centers of two laterally adjacent slots is shorter than the free-space wavelength λo of the transmission wave (i.e., less than about 4 mm), no grating lobes will occur frontward. As a result, influences of grating lobes are reduced. Note that grating lobes will occur when the interval at which the antenna elements are arrayed is greater than a half of the wavelength of an electromagnetic wave. If the interval at which the antenna elements are arrayed is less than the wavelength, no grating lobes will occur frontward. Therefore, in the case where no beam steering is performed to impart phase differences among the radio waves radiated from the respective antenna elements composing an array antenna, grating lobes will exert substantially no influences so long as the interval at which the antenna elements are arrayed is smaller than the wavelength. By adjusting the array factor of the transmission antenna, the directivity of the transmission antenna can be adjusted. A phase shifter may be provided so as to be able to individually adjust the phases of electromagnetic waves that are transmitted on plural waveguide members. In that case, even if the interval between antenna elements is made less than the free-space wavelength λo of the transmission wave, grating lobes will appear as the phase shift amount is increased. However, when the intervals between the antenna elements is reduced to less than a half of the free space wavelength λo of the transmission wave, grating lobes will not appear irrespective of the phase shift amount. By providing a phase shifter, the directivity of the transmission antenna can be changed in any desired direction. Since the construction of a phase shifter is well-known, description thereof will be omitted.

A reception antenna according to the Application Example is able to reduce reception of reflected waves associated with grating lobes, thereby being able to improve the precision of the below-described processing. Hereinafter, an example of a reception process will be described.

FIG. 38A shows a relationship between an array antenna AA of the onboard radar system 510 and plural arriving waves k (k: an integer from 1 to K; the same will always apply below. K is the number of targets that are present in different azimuths). The array antenna AA includes M antenna elements in a linear array. Principlewise, an antenna can be used for both transmission and reception, and therefore the array antenna AA can be used for both a transmission antenna and a reception antenna. Hereinafter, an example method of processing an arriving wave which is received by the reception antenna will be described.

The array antenna AA receives plural arriving waves that simultaneously impinge at various angles. Some of the plural arriving waves may be arriving waves which have been radiated from the transmission antenna of the same onboard radar system 510 and reflected by a target(s). Furthermore, some of the plural arriving waves may be direct or indirect arriving waves that have been radiated from other vehicles.

The incident angle of each arriving wave (i.e., an angle representing its direction of arrival) is an angle with respect to the broadside B of the array antenna AA. The incident angle of an arriving wave represents an angle with respect to a direction which is perpendicular to the direction of the line along which antenna elements are arrayed.

Now, consider a k^(th) arriving wave. Where K arriving waves are impinging on the array antenna from K targets existing at different azimuths, a “k^(th) arriving wave” means an arriving wave which is identified by an incident angle θ_(k).

FIG. 38B shows the array antenna AA receiving the k^(th) arriving wave. The signals received by the array antenna AA can be expressed as a “vector” having M elements, by Math. 1. S=[s ₁ ,s ₂ , . . . ,s _(M)]^(T)  [Math. 1]

In the above, s_(m) (where m is an integer from 1 to M; the same will also be true hereinbelow) is the value of a signal which is received by an m^(th) antenna element. The superscript ^(T) means transposition. S is a column vector. The column vector S is defined by a product of multiplication between a direction vector (referred to as a steering vector or a mode vector) as determined by the construction of the array antenna and a complex vector representing a signal from each target (also referred to as a wave source or a signal source). When the number of wave sources is K, the waves of signals arriving at each individual antenna element from the respective K wave sources are linearly superposed. In this state, s_(m) can be expressed by Math. 2.

$\begin{matrix} {s_{m} = {\sum\limits_{k = 1}^{K}{a_{k}\exp\left\{ {j\left( {{\frac{{2\pi}\;}{\lambda}d_{m}\sin\;\theta_{k}} + \varphi_{k}} \right)} \right\}}}} & \left\lbrack {{Math}.\mspace{14mu} 2} \right\rbrack \end{matrix}$

In Math. 2, a_(k), θ_(k) and φ_(k) respectively denote the amplitude, incident angle, and initial phase of the k^(th) arriving wave. Moreover, λ denotes the wavelength of an arriving wave, and j is an imaginary unit.

As will be understood from Math. 2, s_(m) is expressed as a complex number consisting of a real part (Re) and an imaginary part (Im).

When this is further generalized by taking noise (internal noise or thermal noise) into consideration, the array reception signal X can be expressed as Math. 3. X=S+N  [Math. 3]

N is a vector expression of noise.

The signal processing circuit generates a spatial covariance matrix Rxx (Math. 4) of arriving waves by using the array reception signal X expressed by Math. 3, and further determines eigenvalues of the spatial covariance matrix Rxx.

$\begin{matrix} \begin{matrix} {R_{xx} = {XX}^{H}} \\ {= \begin{bmatrix} {Rxx}_{11} & \ldots & {Rxx}_{1M} \\ \vdots & \ddots & \vdots \\ {Rxx}_{M\; 1} & \ldots & {Rxx}_{MM} \end{bmatrix}} \end{matrix} & \left\lbrack {{Math}.\mspace{14mu} 4} \right\rbrack \end{matrix}$

In the above, the superscript H means complex conjugate transposition (Hermitian conjugate).

Among the eigenvalues, the number of eigenvalues which have values equal to or greater than a predetermined value that is defined based on thermal noise (signal space eigenvalues) corresponds to the number of arriving waves. Then, angles that produce the highest likelihood as to the directions of arrival of reflected waves (i.e. maximum likelihood) are calculated, whereby the number of targets and the angles at which the respective targets are present can be identified. This process is known as a maximum likelihood estimation technique.

Next, see FIG. 39. FIG. 39 is a block diagram showing an exemplary fundamental construction of a vehicle travel controlling apparatus 600 according to the present disclosure. The vehicle travel controlling apparatus 600 shown in FIG. 39 includes a radar system 510 which is mounted in a vehicle, and a travel assistance electronic control apparatus 520 which is connected to the radar system 510. The radar system 510 includes an array antenna AA and a radar signal processing apparatus 530.

The array antenna AA includes a plurality of antenna elements, each of which outputs a reception signal in response to one or plural arriving waves. As mentioned earlier, the array antenna AA is capable of radiating a millimeter wave of a high frequency.

In the radar system 510, the array antenna AA needs to be attached to the vehicle, while at least some of the functions of the radar signal processing apparatus 530 may be implemented by a computer 550 and a database 552 which are provided externally to the vehicle travel controlling apparatus 600 (e.g., outside of the driver's vehicle). In that case, the portions of the radar signal processing apparatus 530 that are located within the vehicle may be perpetually or occasionally connected to the computer 550 and database 552 external to the vehicle so that bidirectional communications of signal or data are possible. The communications are to be performed via a communication device 540 of the vehicle and a commonly-available communications network.

The database 552 may store a program which defines various signal processing algorithms. The content of the data and program needed for the operation of the radar system 510 may be externally updated via the communication device 540. Thus, at least some of the functions of the radar system 510 can be realized externally to the driver's vehicle (which is inclusive of the interior of another vehicle), by a cloud computing technique. Therefore, an “onboard” radar system in the meaning of the present disclosure does not require that all of its constituent elements be mounted within the (driver's) vehicle. However, for simplicity, the present application will describe an implementation in which all constituent elements according to the present disclosure are mounted in a single vehicle (i.e., the driver's vehicle), unless otherwise specified.

The radar signal processing apparatus 530 includes a signal processing circuit 560. The signal processing circuit 560 directly or indirectly receives reception signals from the array antenna AA, and inputs the reception signals, or a secondary signal(s) which has been generated from the reception signals, to an arriving wave estimation unit AU. A part or a whole of the circuit (not shown) which generates a secondary signal(s) from the reception signals does not need to be provided inside of the signal processing circuit 560. A part or a whole of such a circuit (preprocessing circuit) may be provided between the array antenna AA and the radar signal processing apparatus 530.

The signal processing circuit 560 is configured to perform computation by using the reception signals or secondary signal(s), and output a signal indicating the number of arriving waves. As used herein, a “signal indicating the number of arriving waves” can be said to be a signal indicating the number of preceding vehicles (which may be one preceding vehicle or plural preceding vehicles) ahead of the driver's vehicle.

The signal processing circuit 560 may be configured to execute various signal processing which is executable by known radar signal processing apparatuses. For example, the signal processing circuit 560 may be configured to execute “super-resolution algorithms” such as the MUSIC method, the ESPRIT method, or the SAGE method, or other algorithms for direction-of-arrival estimation of relatively low resolution.

The arriving wave estimation unit AU shown in FIG. 39 estimates an angle representing the azimuth of each arriving wave by an arbitrary algorithm for direction-of-arrival estimation, and outputs a signal indicating the estimation result. The signal processing circuit 560 estimates the distance to each target as a wave source of an arriving wave, the relative velocity of the target, and the azimuth of the target by using a known algorithm which is executed by the arriving wave estimation unit AU, and output a signal indicating the estimation result.

In the present disclosure, the term “signal processing circuit” is not limited to a single circuit, but encompasses any implementation in which a combination of plural circuits is conceptually regarded as a single functional part. The signal processing circuit 560 may be realized by one or more System-on-Chips (SoCs). For example, a part or a whole of the signal processing circuit 560 may be an FPGA (Field-Programmable Gate Array), which is a programmable logic device (PLD). In that case, the signal processing circuit 560 includes a plurality of computation elements (e.g., general-purpose logics and multipliers) and a plurality of memory elements (e.g., look-up tables or memory blocks). Alternatively, the signal processing circuit 560 may be a set of a general-purpose processor(s) and a main memory device(s). The signal processing circuit 560 may be a circuit which includes a processor core(s) and a memory device(s). These may function as the signal processing circuit 560.

The travel assistance electronic control apparatus 520 is configured to provide travel assistance for the vehicle based on various signals which are output from the radar signal processing apparatus 530. The travel assistance electronic control apparatus 520 instructs various electronic control units to fulfill predetermined functions, e.g., a function of issuing an alarm to prompt the driver to make a braking operation when the distance to a preceding vehicle (vehicular gap) has become shorter than a predefined value; a function of controlling the brakes; and a function of controlling the accelerator. For example, in the case of an operation mode which performs adaptive cruise control of the driver's vehicle, the travel assistance electronic control apparatus 520 sends predetermined signals to various electronic control units (not shown) and actuators, to maintain the distance of the driver's vehicle to a preceding vehicle at a predefined value, or maintain the traveling velocity of the driver's vehicle at a predefined value.

In the case of the MUSIC method, the signal processing circuit 560 determines eigenvalues of the spatial covariance matrix, and, as a signal indicating the number of arriving waves, outputs a signal indicating the number of those eigenvalues (“signal space eigenvalues”) which are greater than a predetermined value (thermal noise power) that is defined based on thermal noise.

Next, see FIG. 40. FIG. 40 is a block diagram showing another exemplary construction for the vehicle travel controlling apparatus 600. The radar system 510 in the vehicle travel controlling apparatus 600 of FIG. 40 includes an array antenna AA, which includes an array antenna that is dedicated to reception only (also referred to as a reception antenna) Rx and an array antenna that is dedicated to transmission only (also referred to as a transmission antenna) Tx; and an object detection apparatus 570.

At least one of the transmission antenna Tx and the reception antenna Rx has the aforementioned waveguide structure. The transmission antenna Tx radiates a transmission wave, which may be a millimeter wave, for example. The reception antenna Rx that is dedicated to reception only outputs a reception signal in response to one or plural arriving waves (e.g., a millimeter wave(s)).

A transmission/reception circuit 580 sends a transmission signal for a transmission wave to the transmission antenna Tx, and performs “preprocessing” for reception signals of reception waves received at the reception antenna Rx. A part or a whole of the preprocessing may be performed by the signal processing circuit 560 in the radar signal processing apparatus 530. A typical example of preprocessing to be performed by the transmission/reception circuit 580 may be generating a beat signal from a reception signal, and converting a reception signal of analog format into a reception signal of digital format. In the present specification, a device that includes a transmission antenna, a reception antenna, a transmission/reception circuit, and a waveguide device that allows an electromagnetic wave to propagate between the transmission antenna and reception antenna and the transmission/reception circuit is referred to as “radar device”. A system that includes an object detection apparatus (including a signal processing circuit) in addition to the radar device is referred to as a radar system”.

Note that the radar system according to the present disclosure may, without being limited to the implementation where it is mounted in the driver's vehicle, be used while being fixed on the road or a building.

Next, an example of a more specific construction of the vehicle travel controlling apparatus 600 will be described.

FIG. 41 is a block diagram showing an example of a more specific construction of the vehicle travel controlling apparatus 600. The vehicle travel controlling apparatus 600 shown in FIG. 41 includes a radar system 510 and an onboard camera system 700. The radar system 510 includes an array antenna AA, a transmission/reception circuit 580 which is connected to the array antenna AA, and a signal processing circuit 560.

The onboard camera system 700 includes an onboard camera 710 which is mounted in a vehicle, and an image processing circuit 720 which processes an image or video that is acquired by the onboard camera 710.

The vehicle travel controlling apparatus 600 of this Application Example includes an object detection apparatus 570 which is connected to the array antenna AA and the onboard camera 710, and a travel assistance electronic control apparatus 520 which is connected to the object detection apparatus 570. The object detection apparatus 570 includes a transmission/reception circuit 580 and an image processing circuit 720, in addition to the above-described radar signal processing apparatus 530 (including the signal processing circuit 560). The object detection apparatus 570 detects a target on the road or near the road, by using not only the information which is obtained by the radar system 510 but also the information which is obtained by the image processing circuit 720. For example, while the driver's vehicle is traveling in one of two or more lanes of the same direction, the image processing circuit 720 can distinguish which lane the driver's vehicle is traveling in, and supply that result of distinction to the signal processing circuit 560. When the number and azimuth(s) of preceding vehicles are to be recognized by using a predetermined algorithm for direction-of-arrival estimation (e.g., the MUSIC method), the signal processing circuit 560 is able to provide more reliable information concerning a spatial distribution of preceding vehicles by referring to the information from the image processing circuit 720.

Note that the onboard camera system 700 is an example of a means for identifying which lane the driver's vehicle is traveling in. The lane position of the driver's vehicle may be identified by any other means. For example, by utilizing an ultra-wide band (UWB) technique, it is possible to identify which one of a plurality of lanes the driver's vehicle is traveling in. It is widely known that the ultra-wide band technique is applicable to position measurement and/or radar. Using the ultra-wide band technique enhances the range resolution of the radar, so that, even when a large number of vehicles exist ahead, each individual target can be detected with distinction, based on differences in distance. This makes it possible to accurately identify distance from a guardrail on the road shoulder, or from the median strip. The width of each lane is predefined based on each country's law or the like. By using such information, it becomes possible to identify where the lane in which the driver's vehicle is currently traveling is. Note that the ultra-wide band technique is an example. A radio wave based on any other wireless technique may be used. Moreover, LIDAR (Light Detection and Ranging) may be used together with a radar. LIDAR is sometimes called “laser radar”.

The array antenna AA may be a generic millimeter wave array antenna for onboard use. The transmission antenna Tx in this Application Example radiates a millimeter wave as a transmission wave ahead of the vehicle. A portion of the transmission wave is reflected off a target which is typically a preceding vehicle, whereby a reflected wave occurs from the target being a wave source. A portion of the reflected wave reaches the array antenna (reception antenna) AA as an arriving wave. Each of the plurality of antenna elements of the array antenna AA outputs a reception signal in response to one or plural arriving waves. In the case where the number of targets functioning as wave sources of reflected waves is K (where K is an integer of one or more), the number of arriving waves is K, but this number K of arriving waves is not known beforehand.

The example of FIG. 39 assumes that the radar system 510 is provided as an integral piece, including the array antenna AA, on the rearview mirror. However, the number and positions of array antennas AA are not limited to any specific number or specific positions. An array antenna AA may be disposed on the rear surface of the vehicle so as to be able to detect targets that are behind the vehicle. Moreover, a plurality of array antennas AA may be disposed on the front surface and the rear surface of the vehicle. The array antenna(s) AA may be disposed inside the vehicle. Even in the case where a horn antenna whose respective antenna elements include horns as mentioned above is to be adopted as the array antenna(s) AA, the array antenna(s) with such antenna elements may be situated inside the vehicle.

The signal processing circuit 560 receives and processes the reception signals which have been received by the reception antenna Rx and subjected to preprocessing by the transmission/reception circuit 580. This process encompasses inputting the reception signals to the arriving wave estimation unit AU, or alternatively, generating a secondary signal(s) from the reception signals and inputting the secondary signal(s) to the arriving wave estimation unit AU.

In the example of FIG. 41, a selection circuit 596 which receives the signal being output from the signal processing circuit 560 and the signal being output from the image processing circuit 720 is provided in the object detection apparatus 570. The selection circuit 596 allows one or both of the signal being output from the signal processing circuit 560 and the signal being output from the image processing circuit 720 to be fed to the travel assistance electronic control apparatus 520.

FIG. 42 is a block diagram showing a more detailed exemplary construction of the radar system 510 according to this Application Example.

As shown in FIG. 42, the array antenna AA includes a transmission antenna Tx which transmits a millimeter wave and reception antennas Rx which receive arriving waves reflected from targets. Although only one transmission antenna Tx is illustrated in the figure, two or more kinds of transmission antennas with different characteristics may be provided. The array antenna AA includes M antenna elements 11 ₁, 11 ₂, . . . , 11 _(M) (where M is an integer of 3 or more). In response to the arriving waves, the plurality of antenna elements 11 ₁, 11 ₂, . . . , 11 _(M) respectively output reception signals s₁, s₂, . . . , s_(M) (FIG. 38B).

In the array antenna AA, the antenna elements 11 ₁ to 11 _(M) are arranged in a linear array or a two-dimensional array at fixed intervals, for example. Each arriving wave will impinge on the array antenna AA from a direction at an angle θ with respect to the normal of the plane in which the antenna elements 11 ₁ to 11 _(M) are arrayed. Thus, the direction of arrival of an arriving wave is defined by this angle θ.

When an arriving wave from one target impinges on the array antenna AA, this approximates to a plane wave impinging on the antenna elements 11 ₁ to 11 _(M) from azimuths of the same angle θ. When K arriving waves impinge on the array antenna AA from K targets with different azimuths, the individual arriving waves can be identified in terms of respectively different angles θ₁ to θ_(K).

As shown in FIG. 42, the object detection apparatus 570 includes the transmission/reception circuit 580 and the signal processing circuit 560.

The transmission/reception circuit 580 includes a triangular wave generation circuit 581, a VCO (voltage controlled oscillator) 582, a distributor 583, mixers 584, filters 585, a switch 586, an A/D converter 587, and a controller 588. Although the radar system in this Application Example is configured to perform transmission and reception of millimeter waves by the FMCW method, the radar system of the present disclosure is not limited to this method. The transmission/reception circuit 580 is configured to generate a beat signal based on a reception signal from the array antenna AA and a transmission signal from the transmission antenna Tx.

The signal processing circuit 560 includes a distance detection section 533, a velocity detection section 534, and an azimuth detection section 536. The signal processing circuit 560 is configured to process a signal from the A/D converter 587 in the transmission/reception circuit 580, and output signals respectively indicating the detected distance to the target, the relative velocity of the target, and the azimuth of the target.

First, the construction and operation of the transmission/reception circuit 580 will be described in detail.

The triangular wave generation circuit 581 generates a triangular wave signal, and supplies it to the VCO 582. The VCO 582 outputs a transmission signal having a frequency as modulated based on the triangular wave signal. FIG. 43 is a diagram showing change in frequency of a transmission signal which is modulated based on the signal that is generated by the triangular wave generation circuit 581. This waveform has a modulation width Δf and a center frequency of f0. The transmission signal having a thus modulated frequency is supplied to the distributor 583. The distributor 583 allows the transmission signal obtained from the VCO 582 to be distributed among the mixers 584 and the transmission antenna Tx. Thus, the transmission antenna radiates a millimeter wave having a frequency which is modulated in triangular waves, as shown in FIG. 43.

In addition to the transmission signal, FIG. 43 also shows an example of a reception signal from an arriving wave which is reflected from a single preceding vehicle. The reception signal is delayed from the transmission signal. This delay is in proportion to the distance between the driver's vehicle and the preceding vehicle. Moreover, the frequency of the reception signal increases or decreases in accordance with the relative velocity of the preceding vehicle, due to the Doppler effect.

When the reception signal and the transmission signal are mixed, a beat signal is generated based on their frequency difference. The frequency of this beat signal (beat frequency) differs between a period in which the transmission signal increases in frequency (ascent) and a period in which the transmission signal decreases in frequency (descent). Once a beat frequency for each period is determined, based on such beat frequencies, the distance to the target and the relative velocity of the target are calculated.

FIG. 44 shows a beat frequency fu in an “ascent” period and a beat frequency fd in a “descent” period. In the graph of FIG. 44, the horizontal axis represents frequency, and the vertical axis represents signal intensity. This graph is obtained by subjecting the beat signal to time-frequency conversion. Once the beat frequencies fu and fd are obtained, based on a known equation, the distance to the target and the relative velocity of the target are calculated. In this Application Example, with the construction and operation described below, beat frequencies corresponding to each antenna element of the array antenna AA are obtained, thus enabling estimation of the position information of a target.

In the example shown in FIG. 42, reception signals from channels Ch₁ to Ch_(M) corresponding to the respective antenna elements 11 ₁ to 11 _(M) are each amplified by an amplifier, and input to the corresponding mixers 584. Each mixer 584 mixes the transmission signal into the amplified reception signal. Through this mixing, a beat signal is generated corresponding to the frequency difference between the reception signal and the transmission signal. The generated beat signal is fed to the corresponding filter 585. The filters 585 apply bandwidth control to the beat signals on the channels Ch₁ to Ch_(M), and supply bandwidth-controlled beat signals to the switch 586.

The switch 586 performs switching in response to a sampling signal which is input from the controller 588. The controller 588 may be composed of a microcomputer, for example. Based on a computer program which is stored in a memory such as a ROM, the controller 588 controls the entire transmission/reception circuit 580. The controller 588 does not need to be provided inside the transmission/reception circuit 580, but may be provided inside the signal processing circuit 560. In other words, the transmission/reception circuit 580 may operate in accordance with a control signal from the signal processing circuit 560. Alternatively, some or all of the functions of the controller 588 may be realized by a central processing unit which controls the entire transmission/reception circuit 580 and signal processing circuit 560.

The beat signals on the channels Ch₁ to Ch_(M) having passed through the respective filters 585 are consecutively supplied to the A/D converter 587 via the switch 586. In synchronization with the sampling signal, the A/D converter 587 converts the beat signals on the channels Ch₁ to Ch_(M), which are input from the switch 586, into digital signals.

Hereinafter, the construction and operation of the signal processing circuit 560 will be described in detail. In this Application Example, the distance to the target and the relative velocity of the target are estimated by the FMCW method. Without being limited to the FMCW method as described below, the radar system can also be implemented by using other methods, e.g., 2 frequency CW and spread spectrum methods.

In the example shown in FIG. 42, the signal processing circuit 560 includes a memory 531, a reception intensity calculation section 532, a distance detection section 533, a velocity detection section 534, a DBF (digital beam forming) processing section 535, an azimuth detection section 536, a target link processing section 537, a matrix generation section 538, a target output processing section 539, and an arriving wave estimation unit AU. As mentioned earlier, a part or a whole of the signal processing circuit 560 may be implemented by FPGA, or by a set of a general-purpose processor(s) and a main memory device(s). The memory 531, the reception intensity calculation section 532, the DBF processing section 535, the distance detection section 533, the velocity detection section 534, the azimuth detection section 536, the target link processing section 537, and the arriving wave estimation unit AU may be individual parts that are implemented in distinct pieces of hardware, or functional blocks of a single signal processing circuit.

FIG. 45 shows an exemplary implementation in which the signal processing circuit 560 is implemented in hardware including a processor PR and a memory device MD. In the signal processing circuit 560 with this construction, too, a computer program that is stored in the memory device MD may fulfill the functions of the reception intensity calculation section 532, the DBF processing section 535, the distance detection section 533, the velocity detection section 534, the azimuth detection section 536, the target link processing section 537, the matrix generation section 538, and the arriving wave estimation unit AU shown in FIG. 42.

The signal processing circuit 560 in this Application Example is configured to estimate the position information of a preceding vehicle by using each beat signal converted into a digital signal as a secondary signal of the reception signal, and output a signal indicating the estimation result. Hereinafter, the construction and operation of the signal processing circuit 560 in this Application Example will be described in detail.

For each of the channels Ch₁ to Ch_(M), the memory 531 in the signal processing circuit 560 stores a digital signal which is output from the A/D converter 587. The memory 531 may be composed of a generic storage medium such as a semiconductor memory or a hard disk and/or an optical disk.

The reception intensity calculation section 532 applies Fourier transform to the respective beat signals for the channels Ch₁ to Ch_(M) (shown in the lower graph of FIG. 43) that are stored in the memory 531. In the present specification, the amplitude of a piece of complex number data after the Fourier transform is referred to as “signal intensity”. The reception intensity calculation section 532 converts the complex number data of a reception signal from one of the plurality of antenna elements, or a sum of the complex number data of all reception signals from the plurality of antenna elements, into a frequency spectrum. In the resultant spectrum, beat frequencies corresponding to respective peak values, which are indicative of presence and distance of targets (preceding vehicles), can be detected. Taking a sum of the complex number data of the reception signals from all antenna elements will allow the noise components to average out, whereby the S/N ratio is improved.

In the case where there is one target, i.e., one preceding vehicle, as shown in FIG. 44, the Fourier transform will produce a spectrum having one peak value in a period of increasing frequency (the “ascent” period) and one peak value in a period of decreasing frequency (“the descent” period). The beat frequency of the peak value in the “ascent” period is denoted by “fu”, whereas the beat frequency of the peak value in the “descent” period is denoted by “fd”.

From the signal intensities of beat frequencies, the reception intensity calculation section 532 detects any signal intensity that exceeds a predefined value (threshold value), thus determining the presence of a target. Upon detecting a signal intensity peak, the reception intensity calculation section 532 outputs the beat frequencies (fu, fd) of the peak values to the distance detection section 533 and the velocity detection section 534 as the frequencies of the object of interest. The reception intensity calculation section 532 outputs information indicating the frequency modulation width Δf to the distance detection section 533, and outputs information indicating the center frequency f0 to the velocity detection section 534.

In the case where signal intensity peaks corresponding to plural targets are detected, the reception intensity calculation section 532 find associations between the ascents peak values and the descent peak values based on predefined conditions. Peaks which are determined as belonging to signals from the same target are given the same number, and thus are fed to the distance detection section 533 and the velocity detection section 534.

When there are plural targets, after the Fourier transform, as many peaks as there are targets will appear in the ascent portions and the descent portions of the beat signal. In proportion to the distance between the radar and a target, the reception signal will become more delayed and the reception signal in FIG. 43 will shift more toward the right. Therefore, a beat signal will have a greater frequency as the distant between the target and the radar increases.

Based on the beat frequencies fu and fd which are input from the reception intensity calculation section 532, the distance detection section 533 calculates a distance R through the equation below, and supplies it to the target link processing section 537. R={c·T/(2·Δf)}·{(fu+fd)/2}

Moreover, based on the beat frequencies fu and fd being input from the reception intensity calculation section 532, the velocity detection section 534 calculates a relative velocity V through the equation below, and supplies it to the target link processing section 537. V={c/(2·f0)}·{(fu−fd)/2}

In the equation which calculates the distance R and the relative velocity V, c is velocity of light, and T is the modulation period.

Note that the lower limit resolution of distance R is expressed as c/(2Δf). Therefore, as Δf increases, the resolution of distance R increases. In the case where the frequency f0 is in the 76 GHz band, when Δf is set on the order of 660 megahertz (MHz), the resolution of distance R will be on the order of 0.23 meters (m), for example. Therefore, if two preceding vehicles are traveling abreast of each other, it may be difficult with the FMCW method to identify whether there is one vehicle or two vehicles. In such a case, it might be possible to run an algorithm for direction-of-arrival estimation that has an extremely high angular resolution to separate between the azimuths of the two preceding vehicles and enable detection.

By utilizing phase differences between signals from the antenna elements 11 ₁, 11 ₂, . . . , 11 _(M), the DBF processing section 535 allows the incoming complex data corresponding to the respective antenna elements, which has been Fourier transformed with respect to the time axis, to be Fourier transformed with respect to the direction in which the antenna elements are arrayed. Then, the DBF processing section 535 calculates spatial complex number data indicating the spectrum intensity for each angular channel as determined by the angular resolution, and outputs it to the azimuth detection section 536 for the respective beat frequencies.

The azimuth detection section 536 is provided for the purpose of estimating the azimuth of a preceding vehicle. Among the values of spatial complex number data that has been calculated for the respective beat frequencies, the azimuth detection section 536 chooses an angle θ that takes the largest value, and outputs it to the target link processing section 537 as the azimuth at which an object of interest exists.

Note that the method of estimating the angle θ indicating the direction of arrival of an arriving wave is not limited to this example. Various algorithms for direction-of-arrival estimation that have been mentioned earlier can be employed.

The target link processing section 537 calculates absolute values of the differences between the respective values of distance, relative velocity, and azimuth of the object of interest as calculated in the current cycle and the respective values of distance, relative velocity, and azimuth of the object of interest as calculated 1 cycle before, which are read from the memory 531. Then, if the absolute value of each difference is smaller than a value which is defined for the respective value, the target link processing section 537 determines that the target that was detected 1 cycle before and the target detected in the current cycle are an identical target. In that case, the target link processing section 537 increments the count of target link processes, which is read from the memory 531, by one.

If the absolute value of a difference is greater than predetermined, the target link processing section 537 determines that a new object of interest has been detected. The target link processing section 537 stores the respective values of distance, relative velocity, and azimuth of the object of interest as calculated in the current cycle and also the count of target link processes for that object of interest to the memory 531.

In the signal processing circuit 560, the distance to the object of interest and its relative velocity can be detected by using a spectrum which is obtained through a frequency analysis of beat signals, which are signals generated based on received reflected waves.

The matrix generation section 538 generates a spatial covariance matrix by using the respective beat signals for the channels Ch₁ to Ch_(M) (lower graph in FIG. 43) stored in the memory 531. In the spatial covariance matrix of Math. 4, each component is the value of a beat signal which is expressed in terms of real and imaginary parts. The matrix generation section 538 further determines eigenvalues of the spatial covariance matrix Rxx, and inputs the resultant eigenvalue information to the arriving wave estimation unit AU.

When a plurality of signal intensity peaks corresponding to plural objects of interest have been detected, the reception intensity calculation section 532 numbers the peak values respectively in the ascent portion and in the descent portion, beginning from those with smaller frequencies first, and output them to the target output processing section 539. In the ascent and descent portions, peaks of any identical number correspond to the same object of interest. The identification numbers are to be regarded as the numbers assigned to the objects of interest. For simplicity of illustration, a leader line from the reception intensity calculation section 532 to the target output processing section 539 is conveniently omitted from FIG. 42.

When the object of interest is a structure ahead, the target output processing section 539 outputs the identification number of that object of interest as indicating a target. When receiving results of determination concerning plural objects of interest, such that all of them are structures ahead, the target output processing section 539 outputs the identification number of an object of interest that is in the lane of the driver's vehicle as the object position information indicating where a target is. Moreover, When receiving results of determination concerning plural objects of interest, such that all of them are structures ahead and that two or more objects of interest are in the lane of the driver's vehicle, the target output processing section 539 outputs the identification number of an object of interest that is associated with the largest count of target being read from the link processes memory 531 as the object position information indicating where a target is.

Referring back to FIG. 41, an example where the onboard radar system 510 is incorporated in the exemplary construction shown in FIG. 41 will be described. The image processing circuit 720 acquires information of an object from the video, and detects target position information from the object information. For example, the image processing circuit 720 is configured to estimate distance information of an object by detecting the depth value of an object within an acquired video, or detect size information and the like of an object from characteristic amounts in the video, thus detecting position information of the object.

The selection circuit 596 selectively feeds position information which is received from the signal processing circuit 560 or the image processing circuit 720 to the travel assistance electronic control apparatus 520. For example, the selection circuit 596 compares a first distance, i.e., the distance from the driver's vehicle to a detected object as contained in the object position information from the signal processing circuit 560, against a second distance, i.e., the distance from the driver's vehicle to the detected object as contained in the object position information from the image processing circuit 720, and determines which is closer to the driver's vehicle. For example, based on the result of determination, the selection circuit 596 may select the object position information which indicates a closer distance to the driver's vehicle, and output it to the travel assistance electronic control apparatus 520. If the result of determination indicates the first distance and the second distance to be of the same value, the selection circuit 596 may output either one, or both of them, to the travel assistance electronic control apparatus 520.

If information indicating that there is no prospective target is input from the reception intensity calculation section 532, the target output processing section 539 (FIG. 42) outputs zero, indicating that there is no target, as the object position information. Then, on the basis of the object position information from the target output processing section 539, through comparison against a predefined threshold value, the selection circuit 596 chooses either the object position information from the signal processing circuit 560 or the object position information from the image processing circuit 720 to be used.

Based on predefined conditions, the travel assistance electronic control apparatus 520 having received the position information of a preceding object from the object detection apparatus 570 performs control to make the operation safer or easier for the driver who is driving the driver's vehicle, in accordance with the distance and size indicated by the object position information, the velocity of the driver's vehicle, road surface conditions such as rainfall, snowfall or clear weather, or other conditions. For example, if the object position information indicates that no object has been detected, the travel assistance electronic control apparatus 520 may send a control signal to an accelerator control circuit 526 to increase speed up to a predefined velocity, thereby controlling the accelerator control circuit 526 to make an operation that is equivalent to stepping on the accelerator pedal.

In the case where the object position information indicates that an object has been detected, if it is found to be at a predetermined distance from the driver's vehicle, the travel assistance electronic control apparatus 520 controls the brakes via a brake control circuit 524 through a brake-by-wire construction or the like. In other words, it makes an operation of decreasing the velocity to maintain a constant vehicular gap. Upon receiving the object position information, the travel assistance electronic control apparatus 520 sends a control signal to an alarm control circuit 522 so as to control lamp illumination or control audio through a loudspeaker which is provided within the vehicle, so that the driver is informed of the nearing of a preceding object. Upon receiving object position information including a spatial distribution of preceding vehicles, the travel assistance electronic control apparatus 520 may, if the traveling velocity is within a predefined range, automatically make the steering wheel easier to operate to the right or left, or control the hydraulic pressure on the steering wheel side so as to force a change in the direction of the wheels, thereby providing assistance in collision avoidance with respect to the preceding object.

The object detection apparatus 570 may be arranged so that, if a piece of object position information which was being continuously detected by the selection circuit 596 for a while in the previous detection cycle but which is not detected in the current detection cycle becomes associated with a piece of object position information from a camera-detected video indicating a preceding object, then continued tracking is chosen, and object position information from the signal processing circuit 560 is output with priority.

An exemplary specific construction and an exemplary operation for the selection circuit 596 to make a selection between the outputs from the signal processing circuit 560 and the image processing circuit 720 are disclosed in the specification of U.S. Pat. No. 8,446,312, the specification of U.S. Pat. No. 8,730,096, and the specification of U.S. Pat. No. 8,730,099. The entire disclosure thereof is incorporated herein by reference.

[First Variant]

In the radar system for onboard use of the above Application Example, the (sweep) condition for a single instance of FMCW (Frequency Modulated Continuous Wave) frequency modulation, i.e., a time span required for such a modulation (sweep time), is e.g. 1 millisecond, although the sweep time could be shortened to about 100 microseconds.

However, in order to realize such a rapid sweep condition, not only the constituent elements involved in the radiation of a transmission wave, but also the constituent elements involved in the reception under that sweep condition must also be able to rapidly operate. For example, an A/D converter 587 (FIG. 42) which rapidly operates under that sweep condition will be needed. The sampling frequency of the A/D converter 587 may be 10 MHz, for example. The sampling frequency may be faster than 10 MHz.

In the present variant, a relative velocity with respect to a target is calculated without utilizing any Doppler shift-based frequency component. In this variant, the sweep time is Tm=100 microseconds, which is very short. The lowest frequency of a detectable beat signal, which is 1/Tm, equals 10 kHz in this case. This would correspond to a Doppler shift of a reflected wave from a target which has a relative velocity of approximately 20 m/second. In other words, so long as one relies on a Doppler shift, it would be impossible to detect relative velocities that are equal to or smaller than this. Thus, a method of calculation which is different from a Doppler shift-based method of calculation is preferably adopted.

As an example, this variant illustrates a process that utilizes a signal (upbeat signal) representing a difference between a transmission wave and a reception wave which is obtained in an upbeat (ascent) portion where the transmission wave increases in frequency. A single sweep time of FMCW is 100 microseconds, and its waveform is a sawtooth shape which is composed only of an upbeat portion. In other words, in this variant, the signal wave which is generated by the triangular wave/CW wave generation circuit 581 has a sawtooth shape. The sweep width in frequency is 500 MHz. Since no peaks are to be utilized that are associated with Doppler shifts, the process is not one that generates an upbeat signal and a downbeat signal to utilize the peaks of both, but will rely on only one of such signals. Although a case of utilizing an upbeat signal will be illustrated herein, a similar process can also be performed by using a downbeat signal.

The A/D converter 587 (FIG. 42) samples each upbeat signal at a sampling frequency of 10 MHz, and outputs several hundred pieces of digital data (hereinafter referred to as “sampling data”). The sampling data is generated based on upbeat signals after a point in time where a reception wave is obtained and until a point in time at which a transmission wave completes transmission, for example. Note that the process may be ended as soon as a certain number of pieces of sampling data are obtained.

In this variant, 128 upbeat signals are transmitted/received in series, for each of which some several hundred pieces of sampling data are obtained. The number of upbeat signals is not limited to 128. It may be 256, or 8. An arbitrary number may be selected depending on the purpose.

The resultant sampling data is stored to the memory 531. The reception intensity calculation section 532 applies a two-dimensional fast Fourier transform (FFT) to the sampling data. Specifically, first, for each of the sampling data pieces that have been obtained through a single sweep, a first FFT process (frequency analysis process) is performed to generate a power spectrum. Next, the velocity detection section 534 performs a second FFT process for the processing results that have been collected from all sweeps.

When the reflected waves are from the same target, peak components in the power spectrum to be detected in each sweep period will be of the same frequency. On the other hand, for different targets, the peak components will differ in frequency. Through the first FFT process, plural targets that are located at different distances can be separated.

In the case where a relative velocity with respect to a target is non-zero, the phase of the upbeat signal changes slightly from sweep to sweep. In other words, through the second FFT process, a power spectrum whose elements are the data of frequency components that are associated with such phase changes will be obtained for the respective results of the first FFT process.

The reception intensity calculation section 532 extracts peak values in the second power spectrum above, and sends them to the velocity detection section 534.

The velocity detection section 534 determines a relative velocity from the phase changes. For example, suppose that a series of obtained upbeat signals undergo phase changes by every phase θ [RXd]. Assuming that the transmission wave has an average wavelength λ, this means there is a λ/(4π/θ) change in distance every time an upbeat signal is obtained. Since this change has occurred over an interval of upbeat signal transmission Tm (=100 microseconds), the relative velocity is determined to be {λ/(4π/θ)}/Tm.

Through the above processes, a relative velocity with respect to a target as well as a distance from the target can be obtained.

[Second Variant]

The radar system 510 is able to detect a target by using a continuous wave(s) CW of one or plural frequencies. This method is especially useful in an environment where a multitude of reflected waves impinge on the radar system 510 from still objects in the surroundings, e.g., when the vehicle is in a tunnel.

The radar system 510 has an antenna array for reception purposes, including five channels of independent reception elements. In such a radar system, the azimuth-of-arrival estimation for incident reflected waves is only possible if there are four or fewer reflected waves that are simultaneously incident. In an FMCW-type radar, the number of reflected waves to be simultaneously subjected to an azimuth-of-arrival estimation can be reduced by exclusively selecting reflected waves from a specific distance. However, in an environment where a large number of still objects exist in the surroundings, e.g., in a tunnel, it is as if there were a continuum of objects to reflect radio waves; therefore, even if one narrows down on the reflected waves based on distance, the number of reflected waves may still not be equal to or smaller than four. However, any such still object in the surroundings will have an identical relative velocity with respect to the driver's vehicle, and the relative velocity will be greater than that associated with any other vehicle that is traveling ahead. On this basis, such still objects can be distinguished from any other vehicle based on the magnitudes of Doppler shifts.

Therefore, the radar system 510 performs a process of: radiating continuous waves CW of plural frequencies; and, while ignoring Doppler shift peaks that correspond to still objects in the reception signals, detecting a distance by using a Doppler shift peak(s) of any smaller shift amount(s). Unlike in the FMCW method, in the CW method, a frequency difference between a transmission wave and a reception wave is ascribable only to a Doppler shift. In other words, any peak frequency that appears in a beat signal is ascribable only to a Doppler shift.

In the description of this variant, too, a continuous wave to be used in the CW method will be referred to as a “continuous wave CW”. As described above, a continuous wave CW has a constant frequency; that is, it is unmodulated.

Suppose that the radar system 510 has radiated a continuous wave CW of a frequency fp, and detected a reflected wave of a frequency fq that has been reflected off a target. The difference between the transmission frequency fp and the reception frequency fq is called a Doppler frequency, which approximates to fp−fq=2·Vr·fp/c. Herein, Vr is a relative velocity between the radar system and the target, and c is the velocity of light. The transmission frequency fp, the Doppler frequency (fp−fq), and the velocity of light c are known. Therefore, from this equation, the relative velocity Vr=(fp−fq)·c/2fp can be determined. The distance to the target is calculated by utilizing phase information as will be described later.

In order to detect a distance to a target by using continuous waves CW, a 2 frequency CW method is adopted. In the 2 frequency CW method, continuous waves CW of two frequencies which are slightly apart are radiated each for a certain period, and their respective reflected waves are acquired. For example, in the case of using frequencies in the 76 GHz band, the difference between the two frequencies would be several hundred kHz. As will be described later, it is more preferable to determine the difference between the two frequencies while taking into account the minimum distance at which the radar used is able to detect a target.

Suppose that the radar system 510 has sequentially radiated continuous waves CW of frequencies fp1 and fp2 (fp1<fp2), and that the two continuous waves CW have been reflected off a single target, resulting in reflected waves of frequencies fq1 and fq2 being received by the radar system 510.

Based on the continuous wave CW of the frequency fp1 and the reflected wave (frequency fq1) thereof, a first Doppler frequency is obtained. Based on the continuous wave CW of the frequency fp2 and the reflected wave (frequency fq2) thereof, a second Doppler frequency is obtained. The two Doppler frequencies have substantially the same value. However, due to the difference between the frequencies fp1 and fp2, the complex signals of the respective reception waves differ in phase. By utilizing this phase information, a distance (range) to the target can be calculated.

Specifically, the radar system 510 is able to determine the distance R as R=c·Δφ/4π(fp2−fp1). Herein, Δφ denotes the phase difference between two beat signals, i.e., beat signal 1 which is obtained as a difference between the continuous wave CW of the frequency fp1 and the reflected wave (frequency fq1) thereof and beat signal 2 which is obtained as a difference between the continuous wave CW of the frequency fp2 and the reflected wave (frequency fq2) thereof. The method of identifying the frequency fb1 of beat signal 1 and the frequency fb2 of beat signal 2 is identical to that in the aforementioned instance of a beat signal from a continuous wave CW of a single frequency.

Note that a relative velocity Vr under the 2 frequency CW method is determined as follows. Vr=fb1·c/2·fp1 or Vr=fb2·c/2·fp2

Moreover, the range in which a distance to a target can be uniquely identified is limited to the range defined by Rmax<c/2(fp2−fp1). The reason is that beat signals resulting from a reflected wave from any farther target would produce a Δφ which is greater than 2n, such that they are indistinguishable from beat signals associated with targets at closer positions. Therefore, it is more preferable to adjust the difference between the frequencies of the two continuous waves CW so that Rmax becomes greater than the minimum detectable distance of the radar. In the case of a radar whose minimum detectable distance is 100 m, fp2−fp1 may be made e.g. 1.0 MHz. In this case, Rmax=150 m, so that a signal from any target from a position beyond Rmax is not detected. In the case of mounting a radar which is capable of detection up to 250 m, fp2−fp1 may be made e.g. 500 kHz. In this case, Rmax=300 m, so that a signal from any target from a position beyond Rmax is not detected, either. In the case where the radar has both of an operation mode in which the minimum detectable distance is 100 m and the horizontal viewing angle is 120 degrees and an operation mode in which the minimum detectable distance is 250 m and the horizontal viewing angle is 5 degrees, it is preferable to switch the fp2−fp1 value be 1.0 MHz and 500 kHz for operation in the respective operation modes.

A detection approach is known which, by transmitting continuous waves CW at N different frequencies (where N is an integer of 3 or more), and utilizing phase information of the respective reflected waves, detects a distance to each target. Under this detection approach, distance can be properly recognized up to N−1 targets. As the processing to enable this, a fast Fourier transform (FFT) is used, for example. Given N=64 or 128, an FFT is performed for sampling data of a beat signal as a difference between a transmission signal and a reception signal for each frequency, thus obtaining a frequency spectrum (relative velocity). Thereafter, at the frequency of the CW wave, a further FFT is performed for peaks of the same frequency, thus to derive distance information.

Hereinafter, this will be described more specifically.

For ease of explanation, first, an instance will be described where signals of three frequencies f1, f2 and f3 are transmitted while being switched over time. It is assumed that f1>f2>f3, and f1−f2=f2−f3=Δf. A transmission time Δt is assumed for the signal wave for each frequency. FIG. 46 shows a relationship between three frequencies f1, f2 and f3.

Via the transmission antenna Tx, the triangular wave/CW wave generation circuit 581 (FIG. 42) transmits continuous waves CW of frequencies f1, f2 and f3, each lasting for the time Δt. The reception antennas Rx receive reflected waves resulting by the respective continuous waves CW being reflected off one or plural targets.

Each mixer 584 mixes a transmission wave and a reception wave to generate a beat signal. The A/D converter 587 converts the beat signal, which is an analog signal, into several hundred pieces of digital data (sampling data), for example.

Using the sampling data, the reception intensity calculation section 532 performs FFT computation. Through the FFT computation, frequency spectrum information of reception signals is obtained for the respective transmission frequencies f1, f2 and f3.

Thereafter, the reception intensity calculation section 532 separates peak values from the frequency spectrum information of the reception signals. The frequency of any peak value which is predetermined or greater is in proportion to a relative velocity with respect to a target. Separating a peak value(s) from the frequency spectrum information of reception signals is synonymous with separating one or plural targets with different relative velocities.

Next, with respect to each of the transmission frequencies f1 to f3, the reception intensity calculation section 532 measures spectrum information of peak values of the same relative velocity or relative velocities within a predefined range.

Now, consider a scenario where two targets A and B exist which have about the same relative velocity but are at respectively different distances. A transmission signal of the frequency f1 will be reflected from both of targets A and B to result in reception signals being obtained. The reflected waves from targets A and B will result in substantially the same beat signal frequency. Therefore, the power spectra at the Doppler frequencies of the reception signals, corresponding to their relative velocities, are obtained as a synthetic spectrum F1 into which the power spectra of two targets A and B have been merged.

Similarly, for each of the frequencies f2 and f3, the power spectra at the Doppler frequencies of the reception signals, corresponding to their relative velocities, are obtained as a synthetic spectrum F1 into which the power spectra of two targets A and B have been merged.

FIG. 47 shows a relationship between synthetic spectra F1 to F3 on a complex plane. In the directions of the two vectors composing each of the synthetic spectra F1 to F3, the right vector corresponds to the power spectrum of a reflected wave from target A; i.e., vectors f1A, f2A and f3A, in FIG. 47. On the other hand, in the directions of the two vectors composing each of the synthetic spectra F1 to F3, the left vector corresponds to the power spectrum of a reflected wave from target B; i.e., vectors f1B, f2B and f3B in FIG. 47.

Under a constant difference Δf between the transmission frequencies, the phase difference between the reception signals corresponding to the respective transmission signals of the frequencies f1 and f2 is in proportion to the distance to a target. Therefore, the phase difference between the vectors f1A and f2A and the phase difference between the vectors f2A and f3A are of the same value θA, this phase difference θA being in proportion to the distance to target A. Similarly, the phase difference between the vectors f1B and f2B and the phase difference between the vectors f2B and f3B are of the same value θB, this phase difference θB being in proportion to the distance to target B.

By using a well-known method, the respective distances to targets A and B can be determined from the synthetic spectra F1 to F3 and the difference Δf between the transmission frequencies. This technique is disclosed in U.S. Pat. No. 6,703,967, for example. The entire disclosure of this publication is incorporated herein by reference.

Similar processing is also applicable when the transmitted signals have four or more frequencies.

Note that, before transmitting continuous waves CW at N different frequencies, a process of determining the distance to and relative velocity of each target may be performed by the 2 frequency CW method. Then, under predetermined conditions, this process may be switched to a process of transmitting continuous waves CW at N different frequencies. For example, FFT computation may be performed by using the respective beat signals at the two frequencies, and if the power spectrum of each transmission frequency undergoes a change over time of 30% or more, the process may be switched. The amplitude of a reflected wave from each target undergoes a large change over time due to multipath influences and the like. When there exists a change of a predetermined magnitude or greater, it may be considered that plural targets may exist.

Moreover, the CW method is known to be unable to detect a target when the relative velocity between the radar system and the target is zero, i.e., when the Doppler frequency is zero. However, when a pseudo Doppler signal is determined by the following methods, for example, it is possible to detect a target by using that frequency.

(Method 1) A mixer that causes a certain frequency shift in the output of a receiving antenna is added. By using a transmission signal and a reception signal with a shifted frequency, a pseudo Doppler signal can be obtained.

(Method 2) A variable phase shifter to introduce phase changes continuously over time is inserted between the output of a receiving antenna and a mixer, thus adding a pseudo phase difference to the reception signal. By using a transmission signal and a reception signal with an added phase difference, a pseudo Doppler signal can be obtained.

An example of specific construction and operation of inserting a variable phase shifter to generate a pseudo Doppler signal under Method 2 is disclosed in Japanese Laid-Open Patent Publication No. 2004-257848. The entire disclosure of this publication is incorporated herein by reference.

When targets with zero or very little relative velocity need to be detected, the aforementioned processes of generating a pseudo Doppler signal may be adopted, or the process may be switched to a target detection process under the FMCW method.

Next, with reference to FIG. 48, a procedure of processing to be performed by the object detection apparatus 570 of the onboard radar system 510 will be described.

The example below will illustrate a case where continuous waves CW are transmitted at two different frequencies fp1 and fp2 (fp1<fp2), and the phase information of each reflected wave is utilized to respectively detect a distance with respect to a target.

FIG. 48 is a flowchart showing the procedure of a process of determining relative velocity and distance according to this variant.

At step S41, the triangular wave/CW wave generation circuit 581 generates two continuous waves CW of frequencies which are slightly apart, i.e., frequencies fp1 and fp2.

At step S42, the transmission antenna Tx and the reception antennas Rx perform transmission/reception of the generated series of continuous waves CW. Note that the process of step S41 and the process of step S42 are to be performed in parallel fashion respectively by the triangular wave/CW wave generation circuit 581 and the transmission antenna Tx/reception antenna Rx, rather than step S42 following only after completion of step S41.

At step S43, each mixer 584 generates a difference signal by utilizing each transmission wave and each reception wave, whereby two difference signals are obtained. Each reception wave is inclusive of a reception wave emanating from a still object and a reception wave emanating from a target. Therefore, next, a process of identifying frequencies to be utilized as the beat signals is performed. Note that the process of step S41, the process of step S42, and the process of step S43 are to be performed in parallel fashion by the triangular wave/CW wave generation circuit 581, the transmission antenna Tx/reception antenna Rx, and the mixers 584, rather than step S42 following only after completion of step S41, or step S43 following only after completion of step S42.

At step S44, for each of the two difference signals, the object detection apparatus 570 identifies certain peak frequencies to be frequencies fb1 and fb2 of beat signals, such that these frequencies are equal to or smaller than a frequency which is predefined as a threshold value and yet they have amplitude values which are equal to or greater than a predetermined amplitude value, and that the difference between the two frequencies is equal to or smaller than a predetermined value.

At step S45, based on one of the two beat signal frequencies identified, the reception intensity calculation section 532 detects a relative velocity. The reception intensity calculation section 532 calculates the relative velocity according to Vr=fb1·c/2·fp1, for example. Note that a relative velocity may be calculated by utilizing each of the two beat signal frequencies, which will allow the reception intensity calculation section 532 to verify whether they match or not, thus enhancing the precision of relative velocity calculation.

At step S46, the reception intensity calculation section 532 determines a phase difference Δφ between two beat signals 1 and 2, and determines a distance R=c·Δφ/4π(fp2−fp1) to the target.

Through the above processes, the relative velocity and distance to a target can be detected.

Note that continuous waves CW may be transmitted at N different frequencies (where N is 3 or more), and by utilizing phase information of the respective reflected wave, distances to plural targets which are of the same relative velocity but at different positions may be detected.

In addition to the radar system 510, the vehicle 500 described above may further include another radar system. For example, the vehicle 500 may further include a radar system having a detection range toward the rear or the sides of the vehicle body. In the case of incorporating a radar system having a detection range toward the rear of the vehicle body, the radar system may monitor the rear, and if there is any danger of having another vehicle bump into the rear, make a response by issuing an alarm, for example. In the case of incorporating a radar system having a detection range toward the sides of the vehicle body, the radar system may monitor an adjacent lane when the driver's vehicle changes its lane, etc., and make a response by issuing an alarm or the like as necessary.

The applications of the above-described radar system 510 are not limited to onboard use only. Rather, the radar system 510 may be used as sensors for various purposes. For example, it may be used as a radar for monitoring the surroundings of a house or any other building. Alternatively, it may be used as a sensor for detecting the presence or absence of a person at a specific indoor place, or whether or not such a person is undergoing any motion, etc., without utilizing any optical images.

[Supplementary Details of Processing]

Other example embodiments will be described in connection with the 2 frequency CW or FMCW techniques for array antennas as described above. As described earlier, in the example of FIG. 42, the reception intensity calculation section 532 applies a Fourier transform to the respective beat signals for the channels Ch₁ to Ch_(M) (lower graph in FIG. 43) stored in the memory 531. These beat signals are complex signals, in order that the phase of the signal of computational interest be identified. This allows the direction of an arriving wave to be accurately identified. In this case, however, the computational load for Fourier transform increases, thus calling for a larger-scaled circuit.

In order to solve this problem, a scalar signal may be generated as a beat signal. For each of a plurality of beat signals that have been generated, two complex Fourier transforms may be performed with respect to the spatial axis direction, which conforms to the antenna array, and to the time axis direction, which conforms to the lapse of time, thus to obtain results of frequency analysis. As a result, with only a small amount of computation, beam formation can eventually be achieved so that directions of arrival of reflected waves can be identified, whereby results of frequency analysis can be obtained for the respective beams. As a patent document related to the present disclosure, the entire disclosure of the specification of U.S. Pat. No. 6,339,395 is incorporated herein by reference.

[Optical Sensor, e.g., Camera, and Millimeter Wave Radar]

Next, a comparison between the above-described array antenna and conventional antennas, as well as an exemplary application in which both of the present array antenna and an optical sensor (e.g., a camera) are utilized, will be described. Note that LIDAR or the like may be employed as the optical sensor.

A millimeter wave radar is able to directly detect a distance (range) to a target and a relative velocity thereof. Another characteristic is that its detection performance is not much deteriorated in the nighttime (including dusk), or in bad weather, e.g., rainfall, fog, or snowfall. On the other hand, it is believed that it is not just as easy for a millimeter wave radar to take a two-dimensional grasp of a target as it is for a camera. On the other hand, it is relatively easy for a camera to take a two-dimensional grasp of a target and recognize its shape. However, a camera may not be able to image a target in nighttime or bad weather, which presents a considerable problem. This problem is particularly outstanding when droplets of water have adhered to the portion through which to ensure lighting, or the eyesight is narrowed by a fog. This problem similarly exists for LIDAR or the like, which also pertains to the realm of optical sensors.

In these years, in answer to increasing demand for safer vehicle operation, driver assist systems for preventing collisions or the like are being developed. A driver assist system acquires an image in the direction of vehicle travel with a sensor such as a camera or a millimeter wave radar, and when any obstacle is recognized that is predicted to hinder vehicle travel, brakes or the like are automatically applied to prevent collisions or the like. Such a function of collision avoidance is expected to operate normally, even in nighttime or bad weather.

Hence, driver assist systems of a so-called fusion construction are gaining prevalence, where, in addition to a conventional optical sensor such as a camera, a millimeter wave radar is mounted as a sensor, thus realizing a recognition process that takes advantage of both. Such a driver assist system will be discussed later.

On the other hand, higher and higher functions are being required of the millimeter wave radar itself. A millimeter wave radar for onboard use mainly uses electromagnetic waves of the 76 GHz band. The antenna power of its antenna is restricted to below a certain level under each country's law or the like. For example, it is restricted to 0.01 W or below in Japan. Under such restrictions, a millimeter wave radar for onboard use is expected to satisfy the required performance that, for example, its detection range is 200 m or more; the antenna size is 60 mm×60 mm or less; its horizontal detection angle is 90 degrees or more; its range resolution is 20 cm or less; it is capable of short-range detection within 10 m; and so on. Conventional millimeter wave radars have used microstrip lines as waveguides, and patch antennas as antennas (hereinafter, these will both be referred to as “patch antennas”). However, with a patch antenna, it has been difficult to attain the aforementioned performance.

By using a slot array antenna to which the technique of the present disclosure is applied, the inventors have successfully achieved the aforementioned performance. As a result, a millimeter wave radar has been realized which is smaller in size, more efficient, and higher-performance than are conventional patch antennas and the like. In addition, by combining this millimeter wave radar and an optical sensor such as a camera, a small-sized, highly efficient, and high-performance fusion apparatus has been realized which has existed never before. This will be described in detail below.

FIG. 49 is a diagram concerning a fusion apparatus in a vehicle 500, the fusion apparatus including an onboard camera system 700 and a radar system 510 (hereinafter referred to also as the millimeter wave radar 510) having a slot array antenna to which the technique of the present disclosure is applied. With reference to this figure, various example embodiments will be described below.

[Installment of Millimeter Wave Radar within Vehicle Room]

A conventional patch antenna-based millimeter wave radar 510′ is placed behind and inward of a grill 512 which is at the front nose of a vehicle. An electromagnetic wave that is radiated from an antenna goes through the apertures in the grill 512, and is radiated ahead of the vehicle 500. In this case, no dielectric layer, e.g., glass, exists that decays or reflects electromagnetic wave energy, in the region through which the electromagnetic wave passes. As a result, an electromagnetic wave that is radiated from the patch antenna-based millimeter wave radar 510′ reaches over a long range, e.g., to a target which is 150 m or farther away. By receiving with the antenna the electromagnetic wave reflected therefrom, the millimeter wave radar 510′ is able to detect a target. In this case, however, since the antenna is placed behind and inward of the grill 512 of the vehicle, the radar may be broken when the vehicle collides into an obstacle. Moreover, it may be soiled with mud or the like in rain, etc., and the soil that has adhered to the antenna may hinder radiation and reception of electromagnetic waves.

Similarly to the conventional manner, the millimeter wave radar 510 incorporating a slot array antenna according to an example embodiment of the present disclosure may be placed behind the grill 512, which is located at the front nose of the vehicle (not shown). This allows the energy of the electromagnetic wave to be radiated from the antenna to be utilized by 100%, thus enabling long-range detection beyond the conventional level, e.g., detection of a target which is at a distance of 250 m or more.

Furthermore, the millimeter wave radar 510 according to an example embodiment of the present disclosure can also be placed within the vehicle room, i.e., inside the vehicle. In that case, the millimeter wave radar 510 is placed inward of the windshield 511 of the vehicle, to fit in a space between the windshield 511 and a face of the rearview mirror (not shown) that is opposite to its specular surface. On the other hand, the conventional patch antenna-based millimeter wave radar 510′ cannot be placed inside the vehicle room mainly for the two following reasons. A first reason is its large size, which prevents itself from being accommodated within the space between the windshield 511 and the rearview mirror. A second reason is that an electromagnetic wave that is radiated ahead reflects off the windshield 511 and decays due to dielectric loss, thus becoming unable to travel the desired distance. As a result, if a conventional patch antenna-based millimeter wave radar is placed within the vehicle room, only targets which are 100 m ahead or less can be detected, for example. On the other hand, a millimeter wave radar according to an example embodiment of the present disclosure is able to detect a target which is at a distance of 200 m or more, despite reflection or decay at the windshield 511. This performance is equivalent to, or even greater than, the case where a conventional patch antenna-based millimeter wave radar is placed outside the vehicle room.

[Fusion Construction Based on Millimeter Wave Radar and Camera, Etc., being Placed within Vehicle Room]

Currently, an optical imaging device such as a CCD camera is used as the main sensor in many a driver assist system (Driver Assist System). Usually, a camera or the like is placed within the vehicle room, inward of the windshield 511, in order to account for unfavorable influences of the external environment, etc. In this context, in order to minimize the optical effect of raindrops and the like, the camera or the like is placed in a region which is swept by the wipers (not shown) but is inward of the windshield 511.

In recent years, due to needs for improved performance of a vehicle in terms of e.g. automatic braking, there has been a desire for automatic braking or the like that is guaranteed to work regardless of whatever external environment may exist. In this case, if the only sensor in the driver assist system is an optical device such as a camera, a problem exists in that reliable operation is not guaranteed in nighttime or bad weather. This has led to the need for a driver assist system that incorporates not only an optical sensor (such as a camera) but also a millimeter wave radar, these being used for cooperative processing, so that reliable operation is achieved even in nighttime or bad weather.

As described earlier, a millimeter wave radar incorporating the present slot array antenna permits itself to be placed within the vehicle room, due to downsizing and remarkable enhancement in the efficiency of the radiated electromagnetic wave over that of a conventional patch antenna. By taking advantage of these properties, as shown in FIG. 49, the millimeter wave radar 510, which incorporates not only an optical sensor (onboard camera system) 700 such as a camera but also a slot array antenna according to the present disclosure, allows both to be placed inward of the windshield 511 of the vehicle 500. This has created the following novel effects.

(1) It is easier to install the driver assist system on the vehicle 500. The conventional patch antenna-based millimeter wave radar 510′ has required a space behind the grill 512, which is at the front nose, in order to accommodate the radar. Since this space may include some sites that affect the structural design of the vehicle, if the size of the radar device is changed, it may have been necessary to reconsider the structural design. This inconvenience is avoided by placing the millimeter wave radar within the vehicle room.

(2) Free from the influences of rain, nighttime, or other external environment factors to the vehicle, more reliable operation can be achieved. Especially, as shown in FIG. 50, by placing the millimeter wave radar (onboard camera system) 510 and the onboard camera system 700 at substantially the same position within the vehicle room, they can attain an identical field of view and line of sight, thus facilitating the “matching process” which will be described later, i.e., a process through which to establish that respective pieces of target information captured by them actually come from an identical object. On the other hand, if the millimeter wave radar 510′ were placed behind the grill 512, which is at the front nose outside the vehicle room, its radar line of sight L would differ from a radar line of sight M of the case where it was placed within the vehicle room, thus resulting in a large offset with the image to be acquired by the onboard camera system 700.

(3) Reliability of the millimeter wave radar device is improved. As described above, since the conventional patch antenna-based millimeter wave radar 510′ is placed behind the grill 512, which is at the front nose, it is likely to gather soil, and may be broken even in a minor collision accident or the like. For these reasons, cleaning and functionality checks are always needed. Moreover, as will be described below, if the position or direction of attachment of the millimeter wave radar becomes shifted due to an accident or the like, it is necessary to reestablish alignment with respect to the camera. The chances of such occurrences are reduced by placing the millimeter wave radar within the vehicle room, whereby the aforementioned inconveniences are avoided.

In a driver assist system of such fusion construction, the optical sensor, e.g., a camera, and the millimeter wave radar 510 incorporating the present slot array antenna may have an integrated construction, i.e., being in fixed position with respect to each other. In that case, certain relative positioning should be kept between the optical axis of the optical sensor such as a camera and the directivity of the antenna of the millimeter wave radar, as will be described later. When this driver assist system having an integrated construction is fixed within the vehicle room of the vehicle 500, the optical axis of the camera, etc., should be adjusted so as to be oriented in a certain direction ahead of the vehicle. For these matters, see US Patent Application Publication No. 2015/0264230, US Patent Application Publication No. 2016/0264065, U.S. patent application Ser. No. 15/248,141, U.S. patent application Ser. No. 15/248,149, and U.S. patent application Ser. No. 15/248,156, which are incorporated herein by reference. Related techniques concerning the camera are described in the specification of U.S. Pat. No. 7,355,524, and the specification of U.S. Pat. No. 7,420,159, the entire disclosure of each which is incorporated herein by reference.

Regarding placement of an optical sensor such as a camera and a millimeter wave radar within the vehicle room, see, for example, the specification of U.S. Pat. No. 8,604,968, the specification of U.S. Pat. No. 8,614,640, and the specification of U.S. Pat. No. 7,978,122, the entire disclosure of each which is incorporated herein by reference. However, at the time when these patents were filed for, only conventional antennas with patch antennas were the known millimeter wave radars, and thus observation was not possible over sufficient distances. For example, the distance that is observable with a conventional millimeter wave radar is considered to be at most 100 m to 150 m. Moreover, when a millimeter wave radar is placed inward of the windshield, the large radar size inconveniently blocks the driver's field of view, thus hindering safe driving. On the other hand, a millimeter wave radar incorporating a slot array antenna according to an example embodiment of the present disclosure is capable of being placed within the vehicle room because of its small size and remarkable enhancement in the efficiency of the radiated electromagnetic wave over that of a conventional patch antenna. This enables a long-range observation over 200 m, while not blocking the driver's field of view.

[Adjustment of Position of Attachment Between Millimeter Wave Radar and Camera, Etc.,]

In the processing under fusion construction (which hereinafter may be referred to as a “fusion process”), it is desired that an image which is obtained with a camera or the like and the radar information which is obtained with the millimeter wave radar map onto the same coordinate system because, if they differ as to position and target size, cooperative processing between both will be hindered.

This involves adjustment from the following three standpoints.

(1) The optical axis of the camera or the like and the antenna directivity of the millimeter wave radar must have a certain fixed relationship.

It is required that the optical axis of the camera or the like and the antenna directivity of the millimeter wave radar are matched. Alternatively, a millimeter wave radar may include two or more transmission antennas and two or more reception antennas, the directivities of these antennas being intentionally made different. Therefore, it is necessary to guarantee that at least a certain known relationship exists between the optical axis of the camera or the like and the directivities of these antennas.

In the case where the camera or the like and the millimeter wave radar have the aforementioned integrated construction, i.e., being in fixed position to each other, the relative positioning between the camera or the like and the millimeter wave radar stays fixed. Therefore, the aforementioned requirements are satisfied with respect to such an integrated construction. On the other hand, in a conventional patch antenna or the like, where the millimeter wave radar is placed behind the grill 512 of the vehicle 500, the relative positioning between them is usually to be adjusted according to (2) below.

(2) A certain fixed relationship exists between an image acquired with the camera or the like and radar information of the millimeter wave radar in an initial state (e.g., upon shipment) of having been attached to the vehicle.

The positions of attachment of the optical sensor such as a camera and the millimeter wave radar 510 or 510′ on the vehicle 500 will finally be determined in the following manner. At a predetermined position 800 ahead of the vehicle 500, a chart to serve as a reference or a target which is subject to observation by the radar (which will hereinafter be referred to as, respectively, a “reference chart” and a “reference target”, and collectively as the “benchmark”) is accurately positioned. This is observed with an optical sensor such as a camera or with the millimeter wave radar 510. The observation information regarding the observed benchmark is compared against previously-stored shape information or the like of the benchmark, and the current offset information is quantitated. Based on this offset information, by at least one of the following means, the positions of attachment of an optical sensor such as a camera and the millimeter wave radar 510 or 510′ are adjusted or corrected. Any other means may also be employed that can provide similar results.

(i) Adjust the positions of attachment of the camera and the millimeter wave radar so that the benchmark will come at a midpoint between the camera and the millimeter wave radar. This adjustment may be done by using a jig or tool, etc., which is separately provided.

(ii) Determine an offset amounts of the camera and the axis/directivity of the millimeter wave radar relative to the benchmark, and through image processing of the camera image and radar processing, correct for these offset amounts in the axis/directivity.

What is to be noted is that, in the case where the optical sensor such as a camera and the millimeter wave radar 510 incorporating a slot array antenna according to an example embodiment of the present disclosure have an integrated construction, i.e., being in fixed position to each other, adjusting an offset of either the camera or the radar with respect to the benchmark will make the offset amount known for the other as well, thus making it unnecessary to check for the other's offset with respect to the benchmark.

Specifically, with respect to the onboard camera system 700, a reference chart may be placed at a predetermined position 750, and an image taken by the camera is compared against advance information indicating where in the field of view of the camera the reference chart image is supposed to be located, thereby detecting an offset amount. Based on this, the camera is adjusted by at least one of the above means (i) and (ii). Next, the offset amount which has been ascertained for the camera is translated into an offset amount of the millimeter wave radar. Thereafter, an offset amount adjustment is made with respect to the radar information, by at least one of the above means (i) and (ii).

Alternatively, this may be performed on the basis of the millimeter wave radar 510. In other words, with respect to the millimeter wave radar 510, a reference target may be placed at a predetermined position 800, and the radar information thereof is compared against advance information indicating where in the field of view of the millimeter wave radar 510 the reference target is supposed to be located, thereby detecting an offset amount. Based on this, the millimeter wave radar 510 is adjusted by at least one of the above means (i) and (ii). Next, the offset amount which has been ascertained for the millimeter wave radar is translated into an offset amount of the camera. Thereafter, an offset amount adjustment is made with respect to the image information obtained by the camera, by at least one of the above means (i) and (ii).

(3) Even after an initial state of the vehicle, a certain relationship is maintained between an image acquired with the camera or the like and radar information of the millimeter wave radar.

Usually, an image acquired with the camera or the like and radar information of the millimeter wave radar are supposed to be fixed in the initial state, and hardly vary unless in an accident of the vehicle or the like. However, if an offset in fact occurs between these, an adjustment is possible by the following means.

The camera is attached in such a manner that portions 513 and 514 (characteristic points) that are characteristic of the driver's vehicle fit within its field of view, for example. The positions at which these characteristic points are actually imaged by the camera are compared against the information of the positions to be assumed by these characteristic points when the camera is attached accurately in place, and an offset amount(s) is detected therebetween. Based on this detected offset amount(s), the position of any image that is taken thereafter may be corrected, whereby an offset of the physical position of attachment of the camera can be corrected for. If this correction sufficiently embodies the performance that is required of the vehicle, then the adjustment per the above (2) may not be needed. By regularly performing this adjustment during startup or operation of the vehicle 500, even if an offset of the camera or the like occurs anew, it is possible to correct for the offset amount, thus helping safe travel.

However, this means is generally considered to result in poorer accuracy of adjustment than with the above means (2). When making an adjustment based on an image which is obtained by imaging a benchmark with the camera, the azimuth of the benchmark can be determined with a high precision, whereby a high accuracy of adjustment can be easily achieved. However, since this means utilizes a part of the vehicle body for the adjustment instead of a benchmark, it is rather difficult to enhance the accuracy of azimuth determination. Thus, the resultant accuracy of adjustment will be somewhat inferior. However, it may still be effective as a means of correction when the position of attachment of the camera or the like is considerably altered for reasons such as an accident or a large external force being applied to the camera or the like within the vehicle room, etc.

[Mapping of Target as Detected by Millimeter Wave Radar and Camera or the Like: Matching Process]

In a fusion process, for a given target, it needs to be established that an image thereof which is acquired with a camera or the like and radar information which is acquired with the millimeter wave radar pertain to “the same target”. For example, suppose that two obstacles (first and second obstacles), e.g., two bicycles, have appeared ahead of the vehicle 500. These two obstacles will be captured as camera images, and detected as radar information of the millimeter wave radar. At this time, the camera image and the radar information with respect to the first obstacle need to be mapped to each other so that they are both directed to the same target. Similarly, the camera image and the radar information with respect to the second obstacle need to be mapped to each other so that they are both directed to the same target. If the camera image of the first obstacle and the radar information of the second obstacle are mistakenly recognized to pertain to an identical object, a considerable accident may occur. Hereinafter, in the present specification, such a process of determining whether a target in the camera image and a target in the radar image pertain to the same target may be referred to as a “matching process”.

This matching process may be implemented by various detection devices (or methods) described below. Hereinafter, these will be specifically described. Note that the each of the following detection devices is to be installed in the vehicle, and at least includes a millimeter wave radar detection section, an image detection section (e.g., a camera) which is oriented in a direction overlapping the direction of detection by the millimeter wave radar detection section, and a matching section. Herein, the millimeter wave radar detection section includes a slot array antenna according to any of the example embodiments of the present disclosure, and at least acquires radar information in its own field of view. The image acquisition section at least acquires image information in its own field of view. The matching section includes a processing circuit which matches a result of detection by the millimeter wave radar detection section against a result of detection by the image detection section to determine whether or not the same target is being detected by the two detection sections. Herein, the image detection section may be composed of a selected one of, or selected two or more of, an optical camera, LIDAR, an infrared radar, and an ultrasonic radar. The following detection devices differ from one another in terms of the detection process at their respective matching section.

In a first detection device, the matching section performs two matches as follows. A first match involves, for a target of interest that has been detected by the millimeter wave radar detection section, obtaining distance information and lateral position information thereof, and also finding a target that is the closest to the target of interest among a target or two or more targets detected by the image detection section, and detecting a combination(s) thereof. A second match involves, for a target of interest that has been detected by the image detection section, obtaining distance information and lateral position information thereof, and also finding a target that is the closest to the target of interest among a target or two or more targets detected by the millimeter wave radar detection section, and detecting a combination(s) thereof. Furthermore, this matching section determines whether there is any matching combination between the combination(s) of such targets as detected by the millimeter wave radar detection section and the combination(s) of such targets as detected by the image detection section. Then, if there is any matching combination, it is determined that the same object is being detected by the two detection sections. In this manner, a match is attained between the respective targets that have been detected by the millimeter wave radar detection section and the image detection section.

A related technique is described in the specification of U.S. Pat. No. 7,358,889, the entire disclosure of which is incorporated herein by reference. In this publication, the image detection section is illustrated by way of a so-called stereo camera that includes two cameras. However, this technique is not limited thereto. In the case where the image detection section includes a single camera, detected targets may be subjected to an image recognition process or the like as appropriate, in order to obtain distance information and lateral position information of the targets. Similarly, a laser sensor such as a laser scanner may be used as the image detection section.

In a second detection device, the matching section matches a result of detection by the millimeter wave radar detection section and a result of detection by the image detection section every predetermined period of time. If the matching section determines that the same target was being detected by the two detection sections in the previous result of matching, it performs a match by using this previous result of matching. Specifically, the matching section matches a target which is currently detected by the millimeter wave radar detection section and a target which is currently detected by the image detection section, against the target which was determined in the previous result of matching to be being detected by the two detection sections. Then, based on the result of matching for the target which is currently detected by the millimeter wave radar detection section and the result of matching for the target which is currently detected by the image detection section, the matching section determines whether or not the same target is being detected by the two detection sections. Thus, rather than directly matching the results of detection by the two detection sections, this detection device performs a chronological match between the two results of detection and a previous result of matching. Therefore, the accuracy of detection is improved over the case of only performing a momentary match, whereby stable matching is realized. In particular, even if the accuracy of the detection section drops momentarily, matching is still possible because of utilizing past results of matching. Moreover, by utilizing the previous result of matching, this detection device is able to easily perform a match between the two detection sections.

In the current match which utilizes the previous result of matching, if the matching section of this detection device determines that the same object is being detected by the two detection sections, then the matching section of this detection device excludes this determined object in performing matching between objects which are currently detected by the millimeter wave radar detection section and objects which are currently detected by the image detection section. Then, this matching section determines whether there exists any identical object that is currently detected by the two detection sections. Thus, while taking into account the result of chronological matching, the detection device also makes a momentary match based on two results of detection that are obtained from moment to moment. As a result, the detection device is able to surely perform a match for any object that is detected during the current detection.

A related technique is described in the specification of U.S. Pat. No. 7,417,580, the entire disclosure of which is incorporated herein by reference. In this publication, the image detection section is illustrated by way of a so-called stereo camera that includes two cameras. However, this technique is not limited thereto. In the case where the image detection section includes a single camera, detected targets may be subjected to an image recognition process or the like as appropriate, in order to obtain distance information and lateral position information of the targets. Similarly, a laser sensor such as a laser scanner may be used as the image detection section.

In a third detection device, the two detection sections and matching section perform detection of targets and performs matches therebetween at predetermined time intervals, and the results of such detection and the results of such matching are chronologically stored to a storage medium, e.g., memory. Then, based on a rate of change in the size of a target in the image as detected by the image detection section, and on a distance to a target from the driver's vehicle and its rate of change (relative velocity with respect to the driver's vehicle) as detected by the millimeter wave radar detection section, the matching section determines whether the target which has been detected by the image detection section and the target which has been detected by the millimeter wave radar detection section are an identical object.

When determining that these targets are an identical object, based on the position of the target in the image as detected by the image detection section, and on the distance to the target from the driver's vehicle and/or its rate of change as detected by the millimeter wave radar detection section, the matching section predicts a possibility of collision with the vehicle.

A related technique is described in the specification of U.S. Pat. No. 6,903,677, the entire disclosure of which is incorporated herein by reference.

As described above, in a fusion process of a millimeter wave radar and an imaging device such as a camera, an image which is obtained with the camera or the like and radar information which is obtained with the millimeter wave radar are matched against each other. A millimeter wave radar incorporating the aforementioned array antenna according to an example embodiment of the present disclosure can be constructed so as to have a small size and high performance. Therefore, high performance and downsizing, etc., can be achieved for the entire fusion process including the aforementioned matching process. This improves the accuracy of target recognition, and enables safer travel control for the vehicle.

[Other Fusion Processes]

In a fusion process, various functions are realized based on a matching process between an image which is obtained with a camera or the like and radar information which is obtained with the millimeter wave radar detection section. Examples of processing apparatuses that realize representative functions of a fusion process will be described below.

Each of the following processing apparatuses is to be installed in a vehicle, and at least includes: a millimeter wave radar detection section to transmit or receive electromagnetic waves in a predetermined direction; an image acquisition section, such as a monocular camera, that has a field of view overlapping the field of view of the millimeter wave radar detection section; and a processing section which obtains information therefrom to perform target detection and the like. The millimeter wave radar detection section acquires radar information in its own field of view. The image acquisition section acquires image information in its own field of view. A selected one, or selected two or more of, an optical camera, LIDAR, an infrared radar, and an ultrasonic radar may be used as the image acquisition section. The processing section can be implemented by a processing circuit which is connected to the millimeter wave radar detection section and the image acquisition section. The following processing apparatuses differ from one another with respect to the content of processing by this processing section.

In a first processing apparatus, the processing section extracts, from an image which is captured by the image acquisition section, a target which is recognized to be the same as the target which is detected by the millimeter wave radar detection section. In other words, a matching process according to the aforementioned detection device is performed. Then, it acquires information of a right edge and a left edge of the extracted target image, and derives locus approximation lines, which are straight lines or predetermined curved lines for approximating loci of the acquired right edge and the left edge, are derived for both edges. The edge which has a larger number of edges existing on the locus approximation line is selected as a true edge of the target. The lateral position of the target is derived on the basis of the position of the edge that has been selected as a true edge. This permits a further improvement on the accuracy of detection of a lateral position of the target.

A related technique is described in the specification of U.S. Pat. No. 8,610,620, the entire disclosure of which is incorporated herein by reference.

In a second processing apparatus, in determining the presence of a target, the processing section alters a determination threshold to be used in checking for a target presence in radar information, on the basis of image information. Thus, if a target image that may be an obstacle to vehicle travel has been confirmed with a camera or the like, or if the presence of a target has been estimated, etc., for example, the determination threshold for the target detection by the millimeter wave radar detection section can be optimized so that more accurate target information can be obtained. In other words, if the possibility of the presence of an obstacle is high, the determination threshold is altered so that this processing apparatus will surely be activated. On the other hand, if the possibility of the presence of an obstacle is low, the determination threshold is altered so that unwanted activation of this processing apparatus is prevented. This permits appropriate activation of the system.

Furthermore in this case, based on radar information, the processing section may designate a region of detection for the image information, and estimate a possibility of the presence of an obstacle on the basis of image information within this region. This makes for a more efficient detection process.

A related technique is described in the specification of U.S. Pat. No. 7,570,198, the entire disclosure of which is incorporated herein by reference.

In a third processing apparatus, the processing section performs combined displaying where images obtained from a plurality of different imaging devices and a millimeter wave radar detection section and an image signal based on radar information are displayed on at least one display device. In this displaying process, horizontal and vertical synchronizing signals are synchronized between the plurality of imaging devices and the millimeter wave radar detection section, and among the image signals from these devices, selective switching to a desired image signal is possible within one horizontal scanning period or one vertical scanning period. This allows, on the basis of the horizontal and vertical synchronizing signals, images of a plurality of selected image signals to be displayed side by side; and, from the display device, a control signal for setting a control operation in the desired imaging device and the millimeter wave radar detection section is sent.

When a plurality of different display devices display respective images or the like, it is difficult to compare the respective images against one another. Moreover, when display devices are provided separately from the third processing apparatus itself, there is poor operability for the device. The third processing apparatus would overcome such shortcomings.

A related technique is described in the specification of U.S. Pat. No. 6,628,299 and the specification of U.S. Pat. No. 7,161,561, the entire disclosure of each of which is incorporated herein by reference.

In a fourth processing apparatus, with respect to a target which is ahead of a vehicle, the processing section instructs an image acquisition section and a millimeter wave radar detection section to acquire an image and radar information containing that target. From within such image information, the processing section determines a region in which the target is contained. Furthermore, the processing section extracts radar information within this region, and detects a distance from the vehicle to the target and a relative velocity between the vehicle and the target. Based on such information, the processing section determines a possibility that the target will collide against the vehicle. This enables an early detection of a possible collision with a target.

A related technique is described in the specification of U.S. Pat. No. 8,068,134, the entire disclosure of which is incorporated herein by reference.

In a fifth processing apparatus, based on radar information or through a fusion process which is based on radar information and image information, the processing section recognizes a target or two or more targets ahead of the vehicle. The “target” encompasses any moving entity such as other vehicles or pedestrians, traveling lanes indicated by white lines on the road, road shoulders and any still objects (including gutters, obstacles, etc.), traffic lights, pedestrian crossings, and the like that may be there. The processing section may encompass a GPS (Global Positioning System) antenna. By using a GPS antenna, the position of the driver's vehicle may be detected, and based on this position, a storage device (referred to as a map information database device) that stores road map information may be searched in order to ascertain a current position on the map. This current position on the map may be compared against a target or two or more targets that have been recognized based on radar information or the like, whereby the traveling environment may be recognized. On this basis, the processing section may extract any target that is estimated to hinder vehicle travel, find safer traveling information, and display it on a display device, as necessary, to inform the driver.

A related technique is described in the specification of U.S. Pat. No. 6,191,704, the entire disclosure of which is incorporated herein by reference.

The fifth processing apparatus may further include a data communication device (having communication circuitry) that communicates with a map information database device which is external to the vehicle. The data communication device may access the map information database device, with a period of e.g. once a week or once a month, to download the latest map information therefrom. This allows the aforementioned processing to be performed with the latest map information.

Furthermore, the fifth processing apparatus may compare between the latest map information that was acquired during the aforementioned vehicle travel and information that is recognized of a target or two or more targets based on radar information, etc., in order to extract target information (hereinafter referred to as “map update information”) that is not included in the map information. Then, this map update information may be transmitted to the map information database device via the data communication device. The map information database device may store this map update information in association with the map information that is within the database, and update the current map information itself, if necessary. In performing the update, respective pieces of map update information that are obtained from a plurality of vehicles may be compared against one another to check certainty of the update.

Note that this map update information may contain more detailed information than the map information which is carried by any currently available map information database device. For example, schematic shapes of roads may be known from commonly-available map information, but it typically does not contain information such as the width of the road shoulder, the width of the gutter that may be there, any newly occurring bumps or dents, shapes of buildings, and so on. Neither does it contain heights of the roadway and the sidewalk, how a slope may connect to the sidewalk, etc. Based on conditions which are separately set, the map information database device may store such detailed information (hereinafter referred to as “map update details information”) in association with the map information. Such map update details information provides a vehicle (including the driver's vehicle) with information which is more detailed than the original map information, thereby rending itself available for not only the purpose of ensuring safe vehicle travel but also some other purposes. As used herein, a “vehicle (including the driver's vehicle)” may be e.g. an automobile, a motorcycle, a bicycle, or any autonomous vehicle to become available in the future, e.g., an electric wheelchair. The map update details information is to be used when any such vehicle may travel.

(Recognition Via Neural Network)

Each of the first to fifth processing apparatuses may further include a sophisticated apparatus of recognition. The sophisticated apparatus of recognition may be provided external to the vehicle. In that case, the vehicle may include a high-speed data communication device that communicates with the sophisticated apparatus of recognition. The sophisticated apparatus of recognition may be constructed from a neural network, which may encompass so-called deep learning and the like. This neural network may include a convolutional neural network (hereinafter referred to as “CNN”), for example. A CNN, a neural network that has proven successful in image recognition, is characterized by possessing one or more sets of two layers, namely, a convolutional layer and a pooling layer.

There exists at least three kinds of information as follows, any of which may be input to a convolutional layer in the processing apparatus:

(1) information that is based on radar information which is acquired by the millimeter wave radar detection section;

(2) information that is based on specific image information which is acquired, based on radar information, by the image acquisition section; or

(3) fusion information that is based on radar information and image information which is acquired by the image acquisition section, or information that is obtained based on such fusion information.

Based on information of any of the above kinds, or information based on a combination thereof, product-sum operations corresponding to a convolutional layer are performed. The results are input to the subsequent pooling layer, where data is selected according to a predetermined rule. In the case of max pooling where a maximum value among pixel values is chosen, for example, the rule may dictate that a maximum value be chosen for each split region in the convolutional layer, this maximum value being regarded as the value of the corresponding position in the pooling layer.

A sophisticated apparatus of recognition that is composed of a CNN may include a single set of a convolutional layer and a pooling layer, or a plurality of such sets which are cascaded in series. This enables accurate recognition of a target, which is contained in the radar information and the image information, that may be around a vehicle.

Related techniques are described in the U.S. Pat. No. 8,861,842, the specification of U.S. Pat. No. 9,286,524, and the specification of US Patent Application Publication No. 2016/0140424, the entire disclosure of each of which is incorporated herein by reference.

In a sixth processing apparatus, the processing section performs processing that is related to headlamp control of a vehicle. When a vehicle travels in nighttime, the driver may check whether another vehicle or a pedestrian exists ahead of the driver's vehicle, and control a beam(s) from the headlamp(s) of the driver's vehicle to prevent the driver of the other vehicle or the pedestrian from being dazzled by the headlamp(s) of the driver's vehicle. This sixth processing apparatus automatically controls the headlamp(s) of the driver's vehicle by using radar information, or a combination of radar information and an image taken by a camera or the like.

Based on radar information, or through a fusion process based on radar information and image information, the processing section detects a target that corresponds to a vehicle or pedestrian ahead of the vehicle. In this case, a vehicle ahead of a vehicle may encompass a preceding vehicle that is ahead, a vehicle or a motorcycle in the oncoming lane, and so on. When detecting any such target, the processing section issues a command to lower the beam(s) of the headlamp(s). Upon receiving this command, the control section (control circuit) which is internal to the vehicle may control the headlamp(s) to lower the beam(s) therefrom.

Related techniques are described in the specification of U.S. Pat. No. 6,403,942, the specification of U.S. Pat. No. 6,611,610, the specification of U.S. Pat. No. 8,543,277, the specification of U.S. Pat. No. 8,593,521, and the specification of U.S. Pat. No. 8,636,393, the entire disclosure of each of which is incorporated herein by reference.

According to the above-described processing by the millimeter wave radar detection section, and the above-described fusion process by the millimeter wave radar detection section and an imaging device such as a camera, the millimeter wave radar can be constructed so as to have a small size and high performance, whereby high performance and downsizing, etc., can be achieved for the radar processing or the entire fusion process. This improves the accuracy of target recognition, and enables safer travel control for the vehicle.

Application Example 2: Various Monitoring Systems (Natural Elements, Buildings, Roads, Watch, Security)

A millimeter wave radar (radar system) incorporating an array antenna according to an example embodiment of the present disclosure also has a wide range of applications in the fields of monitoring, which may encompass natural elements, weather, buildings, security, nursing care, and the like. In a monitoring system in this context, a monitoring apparatus that includes the millimeter wave radar may be installed e.g. at a fixed position, in order to perpetually monitor a subject(s) of monitoring. Regarding the given subject(s) of monitoring, the millimeter wave radar has its resolution of detection adjusted and set to an optimum value.

A millimeter wave radar incorporating an array antenna according to an example embodiment of the present disclosure is capable of detection with a radio frequency electromagnetic wave exceeding e.g. 100 GHz. As for the modulation band in those schemes which are used in radar recognition, e.g., the FMCW method, the millimeter wave radar currently achieves a wide band exceeding 4 GHz, which supports the aforementioned Ultra Wide Band (UWB). Note that the modulation band is related to the range resolution. In a conventional patch antenna, the modulation band was up to about 600 MHz, thus resulting in a range resolution of 25 cm. On the other hand, a millimeter wave radar associated with the present array antenna has a range resolution of 3.75 cm, indicative of a performance which rivals the range resolution of conventional LIDAR. Whereas an optical sensor such as LIDAR is unable to detect a target in nighttime or bad weather as mentioned above, a millimeter wave radar is always capable of detection, regardless of daytime or nighttime and irrespective of weather. As a result, a millimeter wave radar associated with the present array antenna is available for a variety of applications which were not possible with a millimeter wave radar incorporating any conventional patch antenna.

FIG. 51 is a diagram showing an exemplary construction for a monitoring system 1500 based on millimeter wave radar. The monitoring system 1500 based on millimeter wave radar at least includes a sensor section 1010 and a main section 1100. The sensor section 1010 at least includes an antenna 1011 which is aimed at the subject of monitoring 1015, a millimeter wave radar detection section 1012 which detects a target based on a transmitted or received electromagnetic wave, and a communication section (communication circuit) 1013 which transmits detected radar information. The main section 1100 at least includes a communication section (communication circuit) 1103 which receives radar information, a processing section (processing circuit) 1101 which performs predetermined processing based on the received radar information, and a data storage section (storage medium) 1102 in which past radar information and other information that is needed for the predetermined processing, etc., are stored. Telecommunication lines 1300 exist between the sensor section 1010 and the main section 1100, via which transmission and reception of information and commands occur between them. As used herein, the telecommunication lines may encompass any of a general-purpose communications network such as the Internet, a mobile communications network, dedicated telecommunication lines, and so on, for example. Note that the present monitoring system 1500 may be arranged so that the sensor section 1010 and the main section 1100 are directly connected, rather than via telecommunication lines. In addition to the millimeter wave radar, the sensor section 1010 may also include an optical sensor such as a camera. This will permit target recognition through a fusion process which is based on radar information and image information from the camera or the like, thus enabling a more sophisticated detection of the subject of monitoring 1015 or the like.

Hereinafter, examples of monitoring systems embodying these applications will be specifically described.

[Natural Element Monitoring System]

A first monitoring system is a system that monitors natural elements (hereinafter referred to as a “natural element monitoring system”). With reference to FIG. 51, this natural element monitoring system will be described. Subjects of monitoring 1015 of the natural element monitoring system 1500 may be, for example, a river, the sea surface, a mountain, a volcano, the ground surface, or the like. For example, when a river is the subject of monitoring 1015, the sensor section 1010 being secured to a fixed position perpetually monitors the water surface of the river 1015. This water surface information is perpetually transmitted to a processing section 1101 in the main section 1100. Then, if the water surface reaches a certain height or above, the processing section 1101 informs a distinct system 1200 which separately exists from the monitoring system (e.g., a weather observation monitoring system), via the telecommunication lines 1300. Alternatively, the processing section 1101 may send information to a system (not shown) which manages the water gate, whereby the system if instructed to automatically close a water gate, etc. (not shown) which is provided at the river 1015.

The natural element monitoring system 1500 is able to monitor a plurality of sensor sections 1010, 1020, etc., with the single main section 1100. When the plurality of sensor sections are distributed over a certain area, the water levels of rivers in that area can be grasped simultaneously. This allows to make an assessment as to how the rainfall in this area may affect the water levels of the rivers, possibly leading to disasters such as floods. Information concerning this can be conveyed to the distinct system 1200 (e.g., a weather observation monitoring system) via the telecommunication lines 1300. Thus, the distinct system 1200 (e.g., a weather observation monitoring system) is able to utilize the conveyed information for weather observation or disaster prediction in a wider area.

The natural element monitoring system 1500 is also similarly applicable to any natural element other than a river. For example, the subject of monitoring of a monitoring system that monitors tsunamis or storm surges is the sea surface level. It is also possible to automatically open or close the water gate of a seawall in response to a rise in the sea surface level. Alternatively, the subject of monitoring of a monitoring system that monitors landslides to be caused by rainfall, earthquakes, or the like may be the ground surface of a mountainous area, etc.

[Traffic Monitoring System]

A second monitoring system is a system that monitors traffic (hereinafter referred to as a “traffic monitoring system”). The subject of monitoring of this traffic monitoring system may be, for example, a railroad crossing, a specific railroad, an airport runway, a road intersection, a specific road, a parking lot, etc.

For example, when the subject of monitoring is a railroad crossing, the sensor section 1010 is placed at a position where the inside of the crossing can be monitored. In this case, in addition to the millimeter wave radar, the sensor section 1010 may also include an optical sensor such as a camera, which will allow a target (subject of monitoring) to be detected from more perspectives, through a fusion process based on radar information and image information. The target information which is obtained with the sensor section 1010 is sent to the main section 1100 via the telecommunication lines 1300. The main section 1100 collects other information (e.g., train schedule information) that may be needed in a more sophisticated recognition process or control, and issues necessary control instructions or the like based thereon. As used herein, a necessary control instruction may be, for example, an instruction to stop a train when a person, a vehicle, etc. is found inside the crossing when it is closed.

If the subject of monitoring is a runway at an airport, for example, a plurality of sensor sections 1010, 1020, etc., may be placed along the runway so as to set the runway to a predetermined resolution, e.g., a resolution that allows any foreign object on the runway that is 5 cm by 5 cm or larger to be detected. The monitoring system 1500 perpetually monitors the runway, regardless of daytime or nighttime and irrespective of weather. This function is enabled by the very ability of the millimeter wave radar according to an example embodiment of the present disclosure to support UWB. Moreover, since the present millimeter wave radar device can be embodied with a small size, a high resolution, and a low cost, it provides a realistic solution for covering the entire runway surface from end to end. In this case, the main section 1100 keeps the plurality of sensor sections 1010, 1020, etc., under integrated management. If a foreign object is found on the runway, the main section 1100 transmits information concerning the position and size of the foreign object to an air-traffic control system (not shown). Upon receiving this, the air-traffic control system temporarily prohibits takeoff and landing on that runway. In the meantime, the main section 1100 transmits information concerning the position and size of the foreign object to a separately-provided vehicle, which automatically cleans the runway surface, etc., for example. Upon receive this, the cleaning vehicle may autonomously move to the position where the foreign object exists, and automatically remove the foreign object. Once removal of the foreign object is completed, the cleaning vehicle transmits information of the completion to the main section 1100. Then, the main section 1100 again confirms that the sensor section 1010 or the like which has detected the foreign object now reports that “no foreign object exists” and that it is safe now, and informs the air-traffic control system of this. Upon receiving this, the air-traffic control system may lift the prohibition of takeoff and landing from the runway.

Furthermore, in the case where the subject of monitoring is a parking lot, for example, it may be possible to automatically recognize which position in the parking lot is currently vacant. A related technique is described in the specification of U.S. Pat. No. 6,943,726, the entire disclosure of which is incorporated herein by reference.

[Security Monitoring System]

A third monitoring system is a system that monitors a trespasser into a piece of private land or a house (hereinafter referred to as a “security monitoring system”). The subject of monitoring of this security monitoring system may be, for example, a specific region within a piece of private land or a house, etc.

For example, if the subject of monitoring is a piece of private land, the sensor section(s) 1010 may be placed at one position, or two or more positions where the sensor section(s) 1010 is able to monitor it. In this case, in addition to the millimeter wave radar, the sensor section(s) 1010 may also include an optical sensor such as a camera, which will allow a target (subject of monitoring) to be detected from more perspectives, through a fusion process based on radar information and image information. The target information which was obtained by the sensor section 1010(s) is sent to the main section 1100 via the telecommunication lines 1300. The main section 1100 collects other information (e.g., reference data or the like needed to accurately recognize whether the trespasser is a person or an animal such as a dog or a bird) that may be needed in a more sophisticated recognition process or control, and issues necessary control instructions or the like based thereon. As used herein, a necessary control instruction may be, for example, an instruction to sound an alarm or activate lighting that is installed in the premises, and also an instruction to directly report to a person in charge of the premises via mobile telecommunication lines or the like, etc. The processing section 1101 in the main section 1100 may allow an internalized, sophisticated apparatus of recognition (that adopts deep learning or a like technique) to recognize the detected target. Alternatively, such a sophisticated apparatus of recognition may be provided externally, in which case the sophisticated apparatus of recognition may be connected via the telecommunication lines 1300.

A related technique is described in the specification of U.S. Pat. No. 7,425,983, the entire disclosure of which is incorporated herein by reference.

Another example embodiment of such a security monitoring system may be a human monitoring system to be installed at a boarding gate at an airport, a station wicket, an entrance of a building, or the like. The subject of monitoring of such a human monitoring system may be, for example, a boarding gate at an airport, a station wicket, an entrance of a building, or the like.

If the subject of monitoring is a boarding gate at an airport, the sensor section(s) 1010 may be installed in a machine for checking personal belongings at the boarding gate, for example. In this case, there may be two checking methods as follows. In a first method, the millimeter wave radar transmits an electromagnetic wave, and receives the electromagnetic wave as it reflects off a passenger (which is the subject of monitoring), thereby checking personal belongings or the like of the passenger. In a second method, a weak millimeter wave which is radiated from the passenger's own body is received by the antenna, thus checking for any foreign object that the passenger may be hiding. In the latter method, the millimeter wave radar preferably has a function of scanning the received millimeter wave. This scanning function may be implemented by using digital beam forming, or through a mechanical scanning operation. Note that the processing by the main section 1100 may utilize a communication process and a recognition process similar to those in the above-described examples.

[Building Inspection System (Non-Destructive Inspection)]

A fourth monitoring system is a system that monitors or checks the concrete material of a road, a railroad overpass, a building, etc., or the interior of a road or the ground, etc., (hereinafter referred to as a “building inspection system”). The subject of monitoring of this building inspection system may be, for example, the interior of the concrete material of an overpass or a building, etc., or the interior of a road or the ground, etc.

For example, if the subject of monitoring is the interior of a concrete building, the sensor section 1010 is structured so that the antenna 1011 can make scan motions along the surface of a concrete building. As used herein, “scan motions” may be implemented manually, or a stationary rail for the scan motion may be separately provided, upon which to cause the movement by using driving power from an electric motor or the like. In the case where the subject of monitoring is a road or the ground, the antenna 1011 may be installed face-down on a vehicle or the like, and the vehicle may be allowed to travel at a constant velocity, thus creating a “scan motion”. The electromagnetic wave to be used by the sensor section 1010 may be a millimeter wave in e.g. the so-called terahertz region, exceeding 100 GHz. As described earlier, even with an electromagnetic wave over e.g. 100 GHz, an array antenna according to an example embodiment of the present disclosure can be adapted to have smaller losses than do conventional patch antennas or the like. An electromagnetic wave of a higher frequency is able to permeate deeper into the subject of checking, such as concrete, thereby realizing a more accurate non-destructive inspection. Note that the processing by the main section 1100 may also utilize a communication process and a recognition process similar to those in the other monitoring systems described above.

A related technique is described in the specification of U.S. Pat. No. 6,661,367, the entire disclosure of which is incorporated herein by reference.

[Human Monitoring System]

A fifth monitoring system is a system that watches over a person who is subject to nursing care (hereinafter referred to as a “human watch system”). The subject of monitoring of this human watch system may be, for example, a person under nursing care or a patient in a hospital, etc.

For example, if the subject of monitoring is a person under nursing care within a room of a nursing care facility, the sensor section(s) 1010 is placed at one position, or two or more positions inside the room where the sensor section(s) 1010 is able to monitor the entirety of the inside of the room. In this case, in addition to the millimeter wave radar, the sensor section 1010 may also include an optical sensor such as a camera. In this case, the subject of monitoring can be monitored from more perspectives, through a fusion process based on radar information and image information. On the other hand, when the subject of monitoring is a person, from the standpoint of privacy protection, monitoring with a camera or the like may not be appropriate. Therefore, sensor selections must be made while taking this aspect into consideration. Note that target detection by the millimeter wave radar will allow a person, who is the subject of monitoring, to be captured not by his or her image, but by a signal (which is, as it were, a shadow of the person). Therefore, the millimeter wave radar may be considered as a desirable sensor from the standpoint of privacy protection.

Information of the person under nursing care which has been obtained by the sensor section(s) 1010 is sent to the main section 1100 via the telecommunication lines 1300. The main section 1100 collects other information (e.g., reference data or the like needed to accurately recognize target information of the person under nursing care) that may be needed in a more sophisticated recognition process or control, and issues necessary control instructions or the like based thereon. As used herein, a necessary control instruction may be, for example, an instruction to directly report a person in charge based on the result of detection, etc. The processing section 1101 in the main section 1100 may allow an internalized, sophisticated apparatus of recognition (that adopts deep learning or a like technique) to recognize the detected target. Alternatively, such a sophisticated apparatus of recognition may be provided externally, in which case the sophisticated apparatus of recognition may be connected via the telecommunication lines 1300.

In the case where a person is the subject of monitoring of the millimeter wave radar, at least the two following functions may be added.

A first function is a function of monitoring the heart rate and/or the respiratory rate. In the case of a millimeter wave radar, an electromagnetic wave is able to see through the clothes to detect the position and motions of the skin surface of a person's body. First, the processing section 1101 detects a person who is the subject of monitoring and an outer shape thereof. Next, in the case of detecting a heart rate, for example, a position on the body surface where the heartbeat motions are easy to detect may be identified, and the motions there may be chronologically detected. This allows a heart rate per minute to be detected, for example. The same is also true when detecting a respiratory rate. By using this function, the health status of a person under nursing care can be perpetually checked, thus enabling a higher-quality watch over a person under nursing care.

A second function is a function of fall detection. A person under nursing care such as an elderly person may fall from time to time, due to weakened legs and feet. When a person falls, the velocity or acceleration of a specific site of the person's body, e.g., the head, will reach a certain level or greater. When the subject of monitoring of the millimeter wave radar is a person, the relative velocity or acceleration of the target of interest can be perpetually detected. Therefore, by identifying the head as the subject of monitoring, for example, and chronologically detecting its relative velocity or acceleration, a fall can be recognized when a velocity of a certain value or greater is detected. When recognizing a fall, the processing section 1101 can issue an instruction or the like corresponding to pertinent nursing care assistance, for example.

Note that the sensor section(s) 1010 is secured to a fixed position(s) in the above-described monitoring system or the like. However, the sensor section(s) 1010 can also be installed on a moving entity, e.g., a robot, a vehicle, a flying object such as a drone. As used herein, the vehicle or the like may encompass not only an automobile, but also a smaller sized moving entity such as an electric wheelchair, for example. In this case, this moving entity may include an internal GPS unit which allows its own current position to be always confirmed. In addition, this moving entity may also have a function of further improving the accuracy of its own current position by using map information and the map update information which has been described with respect to the aforementioned fifth processing apparatus.

Furthermore, in any device or system that is similar to the above-described first to third detection devices, first to sixth processing apparatuses, first to fifth monitoring systems, etc., a like construction may be adopted to utilize an array antenna or a millimeter wave radar according to an example embodiment of the present disclosure.

Application Example 3: Communication System

[First Example of Communication System]

The waveguide device and antenna device (array antenna) according to the present disclosure can be used for the transmitter and/or receiver with which a communication system (telecommunication system) is constructed. The waveguide device and antenna device according to the present disclosure are composed of layered conductive members, and therefore are able to keep the transmitter and/or receiver size smaller than in the case of using a hollow waveguide. Moreover, there is no need for dielectric, and thus the dielectric loss of electromagnetic waves can be kept smaller than in the case of using a microstrip line. Therefore, a communication system including a small and highly efficient transmitter and/or receiver can be constructed.

Such a communication system may be an analog type communication system which transmits or receives an analog signal that is directly modulated. However, a digital communication system may be adopted in order to construct a more flexible and higher-performance communication system.

Hereinafter, with reference to FIG. 52, a digital communication system 800A in which a waveguide device and an antenna device according to an example embodiment of the present disclosure are used will be described.

FIG. 52 is a block diagram showing a construction for the digital communication system 800A. The communication system 800A includes a transmitter 810A and a receiver 820A. The transmitter 810A includes an analog to digital (A/D) converter 812, an encoder 813, a modulator 814, and a transmission antenna 815. The receiver 820A includes a reception antenna 825, a demodulator 824, a decoder 823, and a digital to analog (D/A) converter 822. The at least one of the transmission antenna 815 and the reception antenna 825 may be implemented by using an array antenna according to an example embodiment of the present disclosure. In this exemplary application, the circuitry including the modulator 814, the encoder 813, the A/D converter 812, and so on, which are connected to the transmission antenna 815, is referred to as the transmission circuit. The circuitry including the demodulator 824, the decoder 823, the D/A converter 822, and so on, which are connected to the reception antenna 825, is referred to as the reception circuit. The transmission circuit and the reception circuit may be collectively referred to as the communication circuit.

With the analog to digital (A/D) converter 812, the transmitter 810A converts an analog signal which is received from the signal source 811 to a digital signal. Next, the digital signal is encoded by the encoder 813. As used herein, “encoding” means altering the digital signal to be transmitted into a format which is suitable for communication. Examples of such encoding include CDM (Code-Division Multiplexing) and the like. Moreover, any conversion for effecting TDM (Time-Division Multiplexing) or FDM (Frequency Division Multiplexing), or OFDM (Orthogonal Frequency Division Multiplexing) is also an example of encoding. The encoded signal is converted by the modulator 814 into a radio frequency signal, so as to be transmitted from the transmission antenna 815.

In the field of communications, a wave representing a signal to be superposed on a carrier wave may be referred to as a “signal wave”; however, the term “signal wave” as used in the present specification does not carry that definition. A “signal wave” as referred to in the present specification is broadly meant to be any electromagnetic wave to propagate in a waveguide, or any electromagnetic wave for transmission/reception via an antenna element.

The receiver 820A restores the radio frequency signal that has been received by the reception antenna 825 to a low frequency signal at the demodulator 824, and to a digital signal at the decoder 823. The decoded digital signal is restored to an analog signal by the digital to analog (D/A) converter 822, and is sent to a data sink (data receiver) 821. Through the above processes, a sequence of transmission and reception processes is completed.

When the communicating agent is a digital appliance such as a computer, analog to digital conversion of the transmission signal and digital to analog conversion of the reception signal are not needed in the aforementioned processes. Thus, the analog to digital converter 812 and the digital to analog converter 822 in FIG. 52 may be omitted. A system of such construction is also encompassed within a digital communication system.

In a digital communication system, in order to ensure signal intensity or expand channel capacity, various methods may be adopted. Many such methods are also effective in a communication system which utilizes radio waves of the millimeter wave band or the terahertz band.

Radio waves in the millimeter wave band or the terahertz band have higher straightness than do radio waves of lower frequencies, and undergoes less diffraction, i.e., bending around into the shadow side of an obstacle. Therefore, it is not uncommon for a receiver to fail to directly receive a radio wave that has been transmitted from a transmitter. Even in such situations, reflected waves may often be received, but a reflected wave of a radio wave signal is often poorer in quality than is the direct wave, thus making stable reception more difficult. Furthermore, a plurality of reflected waves may arrive through different paths. In that case, the reception waves with different path lengths might differ in phase from one another, thus causing multi-path fading.

As a technique for improving such situations, a so-called antenna diversity technique may be used. In this technique, at least one of the transmitter and the receiver includes a plurality of antennas. If the plurality of antennas are parted by distances which differ from one another by at least about the wavelength, the resulting states of the reception waves will be different. Accordingly, the antenna that is capable of transmission/reception with the highest quality among all is selectively used, thereby enhancing the reliability of communication. Alternatively, signals which are obtained from more than one antenna may be merged for an improved signal quality.

In the communication system 800A shown in FIG. 52, for example, the receiver 820A may include a plurality of reception antennas 825. In this case, a switcher exists between the plurality of reception antennas 825 and the demodulator 824. Through the switcher, the receiver 820A connects the antenna that provides the highest-quality signal among the plurality of reception antennas 825 to the demodulator 824. In this case, the transmitter 810A may also include a plurality of transmission antennas 815.

[Second Example of Communication System]

FIG. 53 is a block diagram showing an example of a communication system 800B including a transmitter 810B which is capable of varying the radiation pattern of radio waves. In this exemplary application, the receiver is identical to the receiver 820A shown in FIG. 52; for this reason, the receiver is omitted from illustration in FIG. 53. In addition to the construction of the transmitter 810A, the transmitter 810B also includes an antenna array 815 b, which includes a plurality of antenna elements 8151. The antenna array 815 b may be an array antenna according to an example embodiment of the present disclosure. The transmitter 810B further includes a plurality of phase shifters (PS) 816 which are respectively connected between the modulator 814 and the plurality of antenna elements 8151. In the transmitter 810B, an output of the modulator 814 is sent to the plurality of phase shifters 816, where phase differences are imparted and the resultant signals are led to the plurality of antenna elements 8151. In the case where the plurality of antenna elements 8151 are disposed at equal intervals, if a radio frequency signal whose phase differs by a certain amount with respect to an adjacent antenna element is fed to each antenna element 8151, a main lobe 817 of the antenna array 815 b will be oriented in an azimuth which is inclined from the front, this inclination being in accordance with the phase difference. This method may be referred to as beam forming.

The azimuth of the main lobe 817 may be altered by allowing the respective phase shifters 816 to impart varying phase differences. This method may be referred to as beam steering. By finding phase differences that are conducive to the best transmission/reception state, the reliability of communication can be enhanced. Although the example here illustrates a case where the phase difference to be imparted by the phase shifters 816 is constant between any adjacent antenna elements 8151, this is not limiting. Moreover, phase differences may be imparted so that the radio wave will be radiated in an azimuth which allows not only the direct wave but also reflected waves to reach the receiver.

A method called null steering can also be used in the transmitter 810B. This is a method where phase differences are adjusted to create a state where the radio wave is radiated in no specific direction. By performing null steering, it becomes possible to restrain radio waves from being radiated toward any other receiver to which transmission of the radio wave is not intended. This can avoid interference. Although a very broad frequency band is available to digital communication utilizing millimeter waves or terahertz waves, it is nonetheless preferable to make as efficient a use of the bandwidth as possible. By using null steering, plural instances of transmission/reception can be performed within the same band, whereby efficiency of utility of the bandwidth can be enhanced. A method which enhances the efficiency of utility of the bandwidth by using techniques such as beam forming, beam steering, and null steering may sometimes be referred to as SDMA (Spatial Division Multiple Access).

[Third Example of Communication System]

In order to increase the channel capacity in a specific frequency band, a method called MIMO (Multiple-Input and Multiple Output) may be adopted. Under MIMO, a plurality of transmission antennas and a plurality of reception antennas are used. A radio wave is radiated from each of the plurality of transmission antennas. In one example, respectively different signals may be superposed on the radio waves to be radiated. Each of the plurality of reception antennas receives all of the transmitted plurality of radio waves. However, since different reception antennas will receive radio waves that arrive through different paths, differences will occur among the phases of the received radio waves. By utilizing these differences, it is possible to, at the receiver side, separate the plurality of signals which were contained in the plurality of radio waves.

The waveguide device and antenna device according to the present disclosure can also be used in a communication system which utilizes MIMO. Hereinafter, an example such a communication system will be described.

FIG. 54 is a block diagram showing an example of a communication system 800C implementing a MIMO function. In the communication system 800C, a transmitter 830 includes an encoder 832, a TX-MIMO processor 833, and two transmission antennas 8351 and 8352. A receiver 840 includes two reception antennas 8451 and 8452, an RX-MIMO processor 843, and a decoder 842. Note that the number of transmission antennas and the number of reception antennas may each be greater than two. Herein, for ease of explanation, an example where there are two antennas of each kind will be illustrated. In general, the channel capacity of an MIMO communication system will increase in proportion to the number of whichever is the fewer between the transmission antennas and the reception antennas.

Having received a signal from the data signal source 831, the transmitter 830 encodes the signal at the encoder 832 so that the signal is ready for transmission. The encoded signal is distributed by the TX-MIMO processor 833 between the two transmission antennas 8351 and 8352.

In a processing method according to one example of the MIMO method, the TX-MIMO processor 833 splits a sequence of encoded signals into two, i.e., as many as there are transmission antennas 8352, and sends them in parallel to the transmission antennas 8351 and 8352. The transmission antennas 8351 and 8352 respectively radiate radio waves containing information of the split signal sequences. When there are N transmission antennas, the signal sequence is split into N. The radiated radio waves are simultaneously received by the two reception antennas 8451 and 8452. In other words, in the radio waves which are received by each of the reception antennas 8451 and 8452, the two signals which were split at the time of transmission are mixedly contained. Separation between these mixed signals is achieved by the RX-MIMO processor 843.

The two mixed signals can be separated by paying attention to the phase differences between the radio waves, for example. A phase difference between two radio waves of the case where the radio waves which have arrived from the transmission antenna 8351 are received by the reception antennas 8451 and 8452 is different from a phase difference between two radio waves of the case where the radio waves which have arrived from the transmission antenna 8352 are received by the reception antennas 8451 and 8452. That is, the phase difference between reception antennas differs depending on the path of transmission/reception. Moreover, unless the spatial relationship between a transmission antenna and a reception antenna is changed, the phase difference therebetween remains unchanged. Therefore, based on correlation between reception signals received by the two reception antennas, as shifted by a phase difference which is determined by the path of transmission/reception, it is possible to extract any signal that is received through that path of transmission/reception. The RX-MIMO processor 843 may separate the two signal sequences from the reception signal e.g. by this method, thus restoring the signal sequence before the split. The restored signal sequence still remains encoded, and therefore is sent to the decoder 842 so as to be restored to the original signal there. The restored signal is sent to the data sink 841.

Although the MIMO communication system 800C in this example transmits or receives a digital signal, an MIMO communication system which transmits or receives an analog signal can also be realized. In that case, in addition to the construction of FIG. 54, an analog to digital converter and a digital to analog converter as have been described with reference to FIG. 52 are provided. Note that the information to be used in distinguishing between signals from different transmission antennas is not limited to phase difference information. Generally speaking, for a different combination of a transmission antenna and a reception antenna, the received radio wave may differ not only in terms of phase, but also in scatter, fading, and other conditions. These are collectively referred to as CSI (Channel State Information). CSI may be utilized in distinguishing between different paths of transmission/reception in a system utilizing MIMO.

Note that it is not an essential requirement that the plurality of transmission antennas radiate transmission waves containing respectively independent signals. So long as separation is possible at the reception antenna side, each transmission antenna may radiate a radio wave containing a plurality of signals. Moreover, beam forming may be performed at the transmission antenna side, while a transmission wave containing a single signal, as a synthetic wave of the radio waves from the respective transmission antennas, may be formed at the reception antenna. In this case, too, each transmission antenna is adapted so as to radiate a radio wave containing a plurality of signals.

In this third example, too, as in the first and second examples, various methods such as CDM, FDM, TDM, and OFDM may be used as a method of signal encoding.

In a communication system, a circuit board that implements an integrated circuit (referred to as a signal processing circuit or a communication circuit) for processing signals may be stacked as a layer on the waveguide device and antenna device according to an example embodiment of the present disclosure. Since the waveguide device and antenna device according to an example embodiment of the present disclosure is structured so that plate-like conductive members are layered therein, it is easy to further stack a circuit board thereupon. By adopting such an arrangement, a transmitter and a receiver which are smaller in volume than in the case where a hollow waveguide or the like is employed can be realized.

In the first to third examples of the communication system as described above, each element of a transmitter or a receiver, e.g., an analog to digital converter, a digital to analog converter, an encoder, a decoder, a modulator, a demodulator, a TX-MIMO processor, or an RX-MIMO processor, is illustrated as one independent element in FIGS. 52, 53, and 54; however, these do not need to be discrete. For example, all of these elements may be realized by a single integrated circuit. Alternatively, some of these elements may be combined so as to be realized by a single integrated circuit. Either case qualifies as an example embodiment of the present invention so long as the functions which have been described in the present disclosure are realized thereby.

A waveguide device and an antenna device according to the present disclosure is usable in any technological field that makes use of an antenna. For example, they are available to various applications where transmission/reception of electromagnetic waves of the gigahertz band or the terahertz band is performed. In particular, they may be used in onboard radar systems, various types of monitoring systems, indoor positioning systems, wireless communication systems, etc., where downsizing is desired.

While example embodiments of the present disclosure have been described above, it is to be understood that variations and modifications will be apparent to those skilled in the art without departing from the scope and spirit of the present disclosure. The scope of the present disclosure, therefore, is to be determined solely by the following claims. 

What is claimed is:
 1. A waveguide device comprising: an electrical conductor including an electrically conductive surface; a waveguide including an electrically-conductive waveguide surface opposed to the electrically conductive surface, and extending alongside the electrically conductive surface; and an artificial magnetic conductor extending on two sides of the waveguide; wherein the waveguide includes a first portion extending in one direction and at least two branches extending from one end of the first portion, the at least two branches including a second portion and a third portion that extend in mutually different directions; the waveguide defined by the electrically conductive surface, the waveguide surface, and the artificial magnetic conductor includes an enlarged gap portion at which a gap between the electrically conductive surface and the waveguide surface is locally enlarged; a size of the gap between the electrically conductive surface and the waveguide surface is greater at the enlarged gap portion than at any site on the waveguide that is adjacent to the enlarged gap portion, and is smaller than a distance between the electrically conductive surface and a root of the waveguide; and at least a portion of a junction at which the first portion is joined with the at least two branches of the waveguide overlaps the enlarged gap portion, as seen through in a direction perpendicular to the electrically conductive surface.
 2. The waveguide device of claim 1, wherein a side-surface junction between a side surface of the first portion and a side surface of at least one of the second and third portions is curved.
 3. The waveguide device of claim 1, wherein, as seen through in a direction perpendicular or substantially perpendicular to the electrically conductive surface, an entirety of the junction is located inside the enlarged gap portion.
 4. The waveguide device of claim 1, wherein a side-surface junction between a side surface of the first portion and a side surface of at least one of the second and third portions is curved; and as seen through in a direction perpendicular or substantially perpendicular to the electrically conductive surface, the entire junction is located inside the enlarged gap portion.
 5. The waveguide device of claim 1, wherein the at least two branches include no more than two branches; and as seen through in a direction perpendicular or substantially perpendicular to the electrically conductive surface, an outer edge of the enlarged gap portion reaches an edge of the two branches or the junction on an opposite side from the first portion.
 6. The waveguide device of claim 1, wherein a side-surface junction between a side surface of the first portion and a side surface of at least one of the second and third portions is curved; the at least two branches include no more than two branches; and as seen through in a direction perpendicular or substantially perpendicular to the electrically conductive surface, an outer edge of the enlarged gap portion reaches an edge of the two branches or the junction on an opposite side from the first portion.
 7. The waveguide device of claim 1, wherein a dimension of the enlarged gap portion along a width direction of the first portion is greater than a width of the first portion.
 8. The waveguide device of claim 1, wherein a side-surface junction between a side surface of the first portion and a side surface of at least one of the second and third portions is curved; and a dimension of the enlarged gap portion along a width direction of the first portion is greater than a width of the first portion.
 9. The waveguide device of claim 1, wherein at least one of the waveguide surface and the electrically conductive surface includes a recess at the enlarged gap portion; and a dimension of the recess as measured along a width direction of the first portion is greater than a depth of a bottom of the recess relative to the waveguide surface or the electrically conductive surface around the recess.
 10. The waveguide device of claim 1, wherein at least one of the waveguide surface and the electrically conductive surface includes a recess at the enlarged gap portion; a dimension of the recess as measured along a width direction of the first portion is greater than a depth of a bottom of the recess relative to the waveguide surface or the electrically conductive surface around the recess; and a side-surface junction between a side surface of the first portion and a side surface of at least one of the second and third portions is curved.
 11. The waveguide device of claim 1, wherein the waveguide surface includes a first recess at the enlarged gap portion; the electrically conductive surface includes a second recess at the enlarged gap portion; and a dimension of the first recess and a dimension of the second recess as measured along a width direction of the first portion are each greater than a sum of a depth of a bottom of the first recess relative to any site on the waveguide surface that is around the first recess and a depth of a bottom of the second recess relative to any site on the electrically conductive surface that is around the second recess.
 12. The waveguide device of claim 1, wherein the at least two branches further include a fourth portion which extends in a different direction from directions in which the second and third portions extend.
 13. The waveguide device of claim 1, wherein at the junction where the first to third portions are joined with one another, the waveguide includes a first depression on a side surface opposite to the first portion, the first depression reaching the waveguide surface; and as viewed in a direction perpendicular or substantially perpendicular to the waveguide surface, the first depression overlaps the enlarged gap portion.
 14. The waveguide device of claim 1, wherein at the junction where the first to third portions are joined with one another, the waveguide includes a first depression on a side surface opposite to the first portion, the first depression reaching the waveguide surface; as viewed in a direction perpendicular or substantially perpendicular to the waveguide surface, the first depression overlaps the enlarged gap portion; and a side-surface junction between a side surface of the first portion and a side surface of at least one of the second and third portions is curved.
 15. The waveguide device of claim 1, wherein at the junction where the first to third portions are joined with one another, the waveguide includes a first depression on a side surface opposite to the first portion, the first depression reaching the waveguide surface; as viewed in a direction perpendicular or substantially perpendicular to the waveguide surface, the first depression overlaps the enlarged gap portion; the at least two branches include no more than two branches; and as seen through in a direction perpendicular to the electrically conductive surface, an outer edge of the enlarged gap portion reaches an edge of the two branches or the junction on an opposite side from the first portion.
 16. The waveguide device of claim 1, wherein the second portion includes a second depression on a side surface connecting to one side surface of the first portion, the second depression reaching the waveguide surface; the third portion includes a third depression on a side surface connecting to another side surface of the first portion, the third depression reaching the waveguide surface; as viewed in a direction perpendicular or substantially perpendicular to the waveguide surface, a distance from a point of intersection between the side surface of the first portion and the side surface of the second portion to a center of the second depression is shorter than a length of the second depression along the direction that the second portion extends, and a distance from a point of intersection between the other side surface of the first portion and the side surface of the third portion to a center of the third depression is shorter than a length of the third depression along the direction that the third portion extends.
 17. The waveguide device of claim 1, further comprising another electrical conductor including another electrically conductive surface opposed to the electrically conductive surface of the electrical conductor; wherein the artificial magnetic conductor includes a plurality of electrically conductive rods each including a leading end opposing the electrically conductive surface and a root connected to the other electrically conductive surface.
 18. The waveguide device of claim 1, further comprising another electrical conductor including another electrically conductive surface opposed to the electrically conductive surface of the electrical conductor; wherein the artificial magnetic conductor includes a plurality of electrically conductive rods each including a leading end opposing the electrically conductive surface and a root connected to the other electrically conductive surface; the at least two branches include no more than two branches; and as seen through in a direction perpendicular or substantially perpendicular to the electrically conductive surface, an outer edge of the enlarged gap portion reaches an edge of the two branches or the junction on an opposite side from the first portion.
 19. The waveguide device of claim 1, further comprising an impedance transformer provided on at least one of the waveguide surface of the first portion and the electrically conductive surface opposed to the waveguide surface of the first portion; wherein the impedance transformer allows a capacitance between the waveguide surface and the electrically conductive surface to be increased from a capacitance at any adjacent site; and a length of the impedance transformer as measured from the one end of the first portion along the one direction is equal to or greater than a width of the waveguide surface.
 20. The waveguide device of claim 1, further comprising an impedance transformer provided on at least one of the waveguide surface of the first portion and the electrically conductive surface opposed to the waveguide surface of the first portion; wherein the impedance transformer allows a capacitance between the waveguide surface and the electrically conductive surface to be increased from a capacitance at any adjacent site; a length of the impedance transformer as measured from the one end of the first portion along the one direction is equal to or greater than a width of the waveguide surface; and the impedance transformer makes a distance between the waveguide surface and the electrically conductive surface smaller than at any adjacent site, or makes a width of the waveguide surface greater than at any adjacent site.
 21. An antenna device comprising: the waveguide device of claim 17; and at least one antenna element that is connected to the waveguide device.
 22. An antenna device comprising: the waveguide device of claim 18; and at least one antenna element that is connected to the waveguide device. 